From 9b527dd08418894ac8c6c66cb95f37140bc23c8b Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Thu, 18 Jan 2018 12:00:39 -0700 Subject: [PATCH 01/22] a RAD doxygen branch checkouted from NCAR/master on Jan/17/2018 --- physics/GFS_RRTMG_post.f90 | 3 +- physics/GFS_RRTMG_pre.f90 | 106 +++++++++++++++++++++++++++++++++- physics/GFS_rad_time_vary.f90 | 1 + physics/GFS_radlw_post.f90 | 3 +- physics/GFS_radlw_pre.f90 | 3 +- physics/GFS_radsw_post.f90 | 3 +- physics/GFS_radsw_pre.f90 | 3 +- physics/GFS_radupdate.f90 | 2 + physics/docs/ccpp_dox | 11 +++- physics/radcons.f90 | 4 +- physics/radiation_aerosols.f | 2 +- physics/radiation_astronomy.f | 2 +- physics/radiation_clouds.f | 2 +- physics/radiation_gases.f | 2 +- physics/radiation_surface.f | 2 +- physics/radlw_datatb.f | 4 +- physics/radlw_main.f | 2 +- physics/radlw_param.f | 2 +- physics/radsw_datatb.f | 8 +-- physics/radsw_main.f | 2 +- physics/radsw_param.f | 2 +- 21 files changed, 145 insertions(+), 24 deletions(-) diff --git a/physics/GFS_RRTMG_post.f90 b/physics/GFS_RRTMG_post.f90 index dbb2136cf..b94235f63 100644 --- a/physics/GFS_RRTMG_post.f90 +++ b/physics/GFS_RRTMG_post.f90 @@ -3,7 +3,8 @@ module GFS_RRTMG_post contains -!>\defgroup GFS_RRTMG_post GFS RRTMG Scheme Post +!>\defgroup GFS_RRTMG_post GFS RRTMG Post +!>\ingroup RRTMG !! @{ !> \section arg_table_GFS_RRTMG_post_init Argument Table !! diff --git a/physics/GFS_RRTMG_pre.f90 b/physics/GFS_RRTMG_pre.f90 index 78086ae2e..a44d3e262 100644 --- a/physics/GFS_RRTMG_pre.f90 +++ b/physics/GFS_RRTMG_pre.f90 @@ -1,12 +1,115 @@ !> \file GFS_RRTMG_pre.f90 !! This file contains +!> \defgroup RRTMG GFS RRTMG Shortwave/Longwave Radiation Scheme +!! @{ +!! \brief The GFS radiation scheme +!! \details Radiative processes are among the most complex and +!! computationally intensive parts of all model physics. As an +!! essential component of modeling the atmosphere, radiation directly +!! and indirectly connects all physics processes with model dynamics, +!! and it regulates the overall earth-atmosphere energy exchanges and +!! transformations. +!! +!! The radiation package in GFS physics has standardized component +!! modules (Table 1). The radiation driver module (\ref +!! module_radiation_driver) is the interface with the Interoperable +!! Physics Driver (IPD) for NGGPS, and it has three subroutines called +!! by IPD (Figure 1): +!! - radinit() is called in subroutine nuopc_phys_init to set up +!! radiation related fixed parameters. +!! - radupdate() is called in subroutine nuopc_rad_update to update +!! values between timesteps. +!! - grrad() is called in subroutine nuopc_rad_run, and it is the +!! driver of radiation calculation. +!! \image html ipd_rad.png "Figure 1: Schematic illustration of the communication between the GFS radiation package and IPD " width=10cm +!! +!! The schematic radiation module structure is shown in Table 1. +!! \image html schematic_Rad_mod.png "Table 1: Schematic Radiation Module Structure" width=10cm +!! +!> GFS radiation package is intended to provide a fast and accurate +!! method of determining the total radiative flux at any given +!! location. These calculations provide both the total radiative flux +!! at the ground surface, which is needed to establish the surface +!! energy budget, and the vertical radiative flux divergence, which is +!! used to calculate the radiative heating and cooling rates of a given +!! atmospheric layer. The magnitude of the terms in the surface energy +!! budget can set the stage for moist deep convection and are crucial +!! to the formation of low-level clouds. In addition, the vertical +!! radiative flux divergence can produce substantial cooling, +!! particularly at the tops of clouds, which can have strong dynamical +!! effects on cloud evolution. +!! +!! It uses a correlated-k distribution method and a transmittance lookup +!! table that is linearly scaled by optical depth to achieve high +!! accuracy and efficiency. The algorithm contains 140 unevenly +!! distributed quadrature points (reduced from the original set of 256) +!! to integrate the cumulative probability distribution functions of +!! absorption over 16 spectral bands. It employs the +!! Clough-Kneizys-Davies (CKD_2.4) continuum model (Clough et al. 1992 +!! \cite clough_et_al_1992) to compute absorption by water vapor at the +!! continuum band. Longwave cloud radiative properties external to the +!! RRTM depend on cloud liquid/ice water path and the effective radius +!! of ice particles and water droplets (Hu and Stamnes 1993 \cite +!! hu_and_stamnes_1993; Ebert and Curry 1992 \cite ebert_and_curry_1992). +!! +!! Changes to Radiation Parameterization since 2007: +!! \n The longwave (LW) and the shortwave (SW) radiation +!! parameterizations in NCEP's operational GFS are both modified and +!! optimized versions of the Rapid Radiative Transfer Model for GCMs +!! (RRTMG_LW v2.3 and RRTMG_SW v2.3, respectively) developed at AER +!! (Iacono et al. 2008 \cite iacono_et_al_2008,Mlawer et al. 1997 +!! \cite mlawer_et_al_1997, Iacono et al., 2000 \cite iacono_et_al_2000, +!! Clough et al., 2005 \cite clough_et_al_2005). The LW algorithm +!! contains 140 unevenly distributed g-points (quadrature points) in 16 +!! broad spectral bands, while the SW algorithm includes 112 g-points +!! in 14 bands. In addition to the major atmospheric absorbing gases of +!! ozone, water vapor, and carbon dioxide, the algorithm also includes +!! various minor absorbing species such as methane, nitrous oxide, +!! oxygen, and in the longwave up to four types of halocarbons (CFCs). +!! To represent statistically the unresolved subgrid cloud variability +!! when dealing multi layered clouds, a Monte-Carlo Independent Column +!! Approximation (McICA) method is used in the RRTMG radiative transfer. +!! A maximum-random cloud overlap method is used in both LW and SW +!! radiation calculations. Cloud condensate path and effective radius +!! for water and ice are used for the calculation of cloud-radiative +!! properties. Hu and Stamnes's method (1993) \cite hu_and_stamnes_1993 +!! is used to treat water clouds in both LW and SW parameterizations. +!! For ice clouds. Fu's parameterizations (1996,1998) \cite fu_1996 +!! \cite fu_et_al_1998 are used in the SW and LW, respectively. +!! +!! In the operational GFS, a climatological tropospheric aerosol with +!! a 5-degree horizontal resolution is used in both LW and SW +!! radiations. A generalized spectral mapping formulation was developed +!! to compute radiative properties of various aerosol components for +!! each of the radiation spectral bands. A separate stratospheric +!! volcanic aerosol parameterization was added that is capable of +!! handling volcanic events. In SW, a new table of incoming solar +!! constants is derived covering time period of 1850-2019 (Vandendool, +!! personal communivation). An eleven-year solar cycle approximation +!! will be used for time out of the window period in long term climate +!! simulations. The SW albedo parameterization uses surface vegetation +!! type based seasonal climatology similar to that described in the +!! NCEP OFFICE Note 441 (Hou et al. 2002 \cite hou_et_al_2002) but with +!! a modification in the treatment of solar zenith angle dependency over +!! snow-free land surface (Yang et al. 2008 \cite yang_et_al_2008). +!! Similarly, vegetation type based non-black-body surface emissivity +!! is used for the LW radiation. Concentrations of atmospheric +!! greenhouse gases are either obtained from global network +!! measurements, such as carbon dioxide (CO2), or taking the +!! climatological constants, the actual CO2 value for the forecast time +!! is an estimation based on the most recent five-year observations. In +!! the lower atmosphere (<3km) a monthly mean CO2 distribution in 15 +!! degree horizontal resolution is used, while a global mean monthly +!! value is used in the upper atmosphere. + module GFS_RRTMG_pre public GFS_RRTMG_pre_run contains -!> \defgroup GFS_RRTMG_pre GFS RRTMG Scheme Pre +!> \defgroup GFS_RRTMG_pre GFS RRTMG Pre +!>\ingroup RRTMG !! @{ !! \section arg_table_GFS_RRTMG_pre_init Argument Table !! @@ -613,5 +716,6 @@ end subroutine GFS_RRTMG_pre_finalize !! @} end module GFS_RRTMG_pre +!! @} diff --git a/physics/GFS_rad_time_vary.f90 b/physics/GFS_rad_time_vary.f90 index b57815e7b..31533a29e 100644 --- a/physics/GFS_rad_time_vary.f90 +++ b/physics/GFS_rad_time_vary.f90 @@ -4,6 +4,7 @@ module GFS_rad_time_vary contains !>\defgroup GFS_rad_time_vary GFS RRTMG Update +!!\ingroup RRTMG !! @{ !! \section arg_table_GFS_rad_time_vary_init Argument Table !! diff --git a/physics/GFS_radlw_post.f90 b/physics/GFS_radlw_post.f90 index be2e2ca39..137b867bf 100644 --- a/physics/GFS_radlw_post.f90 +++ b/physics/GFS_radlw_post.f90 @@ -3,7 +3,8 @@ module GFS_radlw_post contains -!>\defgroup GFS_radlw_post GFS RRTMG/RADLW Scheme Post +!>\defgroup GFS_radlw_post GFS RADLW Post +!! \ingroup RRTMG !! @{ !> \section arg_table_GFS_radlw_post_init Argument Table !! diff --git a/physics/GFS_radlw_pre.f90 b/physics/GFS_radlw_pre.f90 index 9d240dff4..9718cd2f0 100644 --- a/physics/GFS_radlw_pre.f90 +++ b/physics/GFS_radlw_pre.f90 @@ -4,7 +4,8 @@ module GFS_radlw_pre contains -!>\defgroup GFS_radlw_pre GFS RADLW Scheme Pre +!>\defgroup GFS_radlw_pre GFS RADLW Pre +!!\ingroup RRTMG !! @{ !> \section arg_table_GFS_radlw_pre_init Argument Table !! diff --git a/physics/GFS_radsw_post.f90 b/physics/GFS_radsw_post.f90 index e391e4938..0dedc17db 100644 --- a/physics/GFS_radsw_post.f90 +++ b/physics/GFS_radsw_post.f90 @@ -3,7 +3,8 @@ module GFS_radsw_post contains -!>\defgroup GFS_radsw_post GFS RRTMG/RADSW Scheme Post +!>\defgroup GFS_radsw_post GFS RADSW Post +!!\ingroup RRTMG !! @{ !> \section arg_table_GFS_radsw_post_init Argument Table !! diff --git a/physics/GFS_radsw_pre.f90 b/physics/GFS_radsw_pre.f90 index bbb583fcf..e672e9889 100644 --- a/physics/GFS_radsw_pre.f90 +++ b/physics/GFS_radsw_pre.f90 @@ -4,7 +4,8 @@ module GFS_radsw_pre contains -!>\defgroup GFS_radsw_pre GFS RADSW Scheme Pre +!>\defgroup GFS_radsw_pre GFS RADSW Pre +!!\ingroup RRTMG !! @{ !> \section arg_table_GFS_radsw_pre_init Argument Table !! diff --git a/physics/GFS_radupdate.f90 b/physics/GFS_radupdate.f90 index b695b618e..fe9349a55 100644 --- a/physics/GFS_radupdate.f90 +++ b/physics/GFS_radupdate.f90 @@ -1,3 +1,5 @@ +!>\file GFS_radupdate.f90 +!! This file contains module GFS_radupdate contains diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index 79b20172c..c594a57c2 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -101,7 +101,6 @@ WARN_FORMAT = WARN_LOGFILE = INPUT = txt/mainpage.txt \ ### Radiation - ../../GFS_layer/GFS_radiation_driver.F90 \ ../radiation_aerosols.f \ ../radiation_astronomy.f \ ../radiation_clouds.f \ @@ -113,6 +112,16 @@ INPUT = txt/mainpage.txt \ ../radsw_datatb.f \ ../radsw_main.f \ ../radsw_param.f \ +### Radiation interstitial + ../GFS_RRTMG_pre.f90 \ + ../GFS_RRTMG_post.f90 \ + ../GFS_radupdate.f90 \ + ../GFS_rad_time_vary.f90 \ + ../GFS_radsw_pre.f90 \ + ../GFS_radsw_post.f90 \ + ../GFS_radlw_pre.f90 \ + ../GFS_radlw_post.f90 \ + ../radcons.f90 \ ### Deep Convection ../mfdeepcnv.f \ ### Shallow Convection diff --git a/physics/radcons.f90 b/physics/radcons.f90 index 1079b07d9..ca01cd46c 100644 --- a/physics/radcons.f90 +++ b/physics/radcons.f90 @@ -2,8 +2,8 @@ !! This file contains module radcons -!> \ingroup rad -!! \defgroup radcons radcons +!> \defgroup radcons GFS RRTMG Contants +!! \ingroup RRTMG !! This module contains some of the most frequently used math and physics !! constants for GCM models. !! @{ diff --git a/physics/radiation_aerosols.f b/physics/radiation_aerosols.f index 23df641c8..2572854d0 100644 --- a/physics/radiation_aerosols.f +++ b/physics/radiation_aerosols.f @@ -116,7 +116,7 @@ !> \ingroup RRTMG -!! \defgroup module_radiation_aerosols module_radiation_aerosols +!! \defgroup module_radiation_aerosols RRTMG Aerosols Module !> @{ !! This module contains climatological atmospheric aerosol schemes for !! radiation computations. diff --git a/physics/radiation_astronomy.f b/physics/radiation_astronomy.f index ac1bbd500..adfc028f1 100644 --- a/physics/radiation_astronomy.f +++ b/physics/radiation_astronomy.f @@ -76,7 +76,7 @@ !> \ingroup RRTMG -!! \defgroup module_radiation_astronomy module_radiation_astronomy +!! \defgroup module_radiation_astronomy RRTMG Astronomy Module !! @{ !> This module sets up astronomical quantities for solar radiation !! calculations. diff --git a/physics/radiation_clouds.f b/physics/radiation_clouds.f index 80b401032..1164c4e31 100644 --- a/physics/radiation_clouds.f +++ b/physics/radiation_clouds.f @@ -146,7 +146,7 @@ !!!!! ========================================================== !!!!! !> \ingroup RRTMG -!! \defgroup module_radiation_clouds module_radiation_clouds +!! \defgroup module_radiation_clouds RRTMG Clouds Module !! @{ !> This module computes cloud related quantities for radiation !! computations. diff --git a/physics/radiation_gases.f b/physics/radiation_gases.f index a2fa97a94..0cac550f5 100644 --- a/physics/radiation_gases.f +++ b/physics/radiation_gases.f @@ -105,7 +105,7 @@ !> \ingroup RRTMG -!! \defgroup module_radiation_gases module_radiation_gases +!! \defgroup module_radiation_gases RRTMG Gases Module !! @{ !> This module sets up ozone climatological profiles and other constant !! gas profiles, such as co2, ch4, n2o, o2, and those of cfc gases. All diff --git a/physics/radiation_surface.f b/physics/radiation_surface.f index f3b8d63c9..d2ca4e79e 100644 --- a/physics/radiation_surface.f +++ b/physics/radiation_surface.f @@ -75,7 +75,7 @@ !> \ingroup RRTMG -!! \defgroup module_radiation_surface module_radiation_surface +!! \defgroup module_radiation_surface RRTMG Surface Module !! @{ !> This module sets up surface albedo for sw radiation and surface !! emissivity for lw radiation. diff --git a/physics/radlw_datatb.f b/physics/radlw_datatb.f index 622b72b03..6918da230 100644 --- a/physics/radlw_datatb.f +++ b/physics/radlw_datatb.f @@ -61,7 +61,7 @@ !!!!! end descriptions !!!!! !!!!! ============================================================== !!!!! -!> \ingroup module_radlw_main +!> \ingroup module_radlw_main !> This module contains plank flux data. !========================================! module module_radlw_avplank ! @@ -738,7 +738,7 @@ module module_radlw_avplank ! end module module_radlw_avplank ! !========================================! -!> \ingroup module_radlw_main +!> \ingroup module_radlw_main !> This module contains reference temperature and pressure. !! !! - These pressures are chosen such that the ln of the first one diff --git a/physics/radlw_main.f b/physics/radlw_main.f index 848c527a0..f132a1e81 100644 --- a/physics/radlw_main.f +++ b/physics/radlw_main.f @@ -235,7 +235,7 @@ !!!!! ============================================================== !!!!! -!> \defgroup module_radlw_main module_radlw_main +!> \defgroup module_radlw_main GFS RADLW Main !! \ingroup RRTMG !! This module includes NCEP's modifications of the rrtmg-lw radiation !! code from AER. diff --git a/physics/radlw_param.f b/physics/radlw_param.f index c76864975..c7a79c68a 100644 --- a/physics/radlw_param.f +++ b/physics/radlw_param.f @@ -1,7 +1,7 @@ !> \file radlw_param.f !! This file contains LW band parameters setup. -!> \ingroup module_radlw_main +!> \ingroup module_radlw_main !! @{ !!!!! ============================================================== !!!!! diff --git a/physics/radsw_datatb.f b/physics/radsw_datatb.f index 7da6132ce..4df54db8b 100644 --- a/physics/radsw_datatb.f +++ b/physics/radsw_datatb.f @@ -63,7 +63,7 @@ !!!!! ============================================================== !!!!! -!> \ingroup module_radlw_main +!> \ingroup module_radsw_main !> This module contains the reference pressures (in logarithm form) at !! 59 vertical levels (TOA is omitted), and the mid-latitude summer !! (MLS) standard temperature profile for the 59 pressure layers that @@ -136,7 +136,7 @@ module module_radsw_ref ! end module module_radsw_ref ! !========================================! -!> \ingroup module_radlw_main +!> \ingroup module_radsw_main !> This module contains cloud radiative property coefficients. !! !! For liquid water clouds, cloud radiative property coefficients are @@ -1924,7 +1924,7 @@ module module_radsw_cldprtb ! end module module_radsw_cldprtb ! !========================================! -!> \ingroup module_radlw_main +!> \ingroup module_radsw_main !> This module contains various indexes and coefficients for SW spectral !! bands, as well as the spectral distribution of solar flux. The values !! of spectral solar flux are derived based on a prescribed solar @@ -2265,7 +2265,7 @@ end module module_radsw_sflux ! !========================================! !>\defgroup module_radsw_kgbnn module_radsw_kgbnn -!>\ingroup module_radsw_main +!>\ingroup module_radsw_main !! @{ !> This module sets up absorption coefficients for band 16: 2600-3250 diff --git a/physics/radsw_main.f b/physics/radsw_main.f index dd28aa2f5..0d50bc3b8 100644 --- a/physics/radsw_main.f +++ b/physics/radsw_main.f @@ -261,7 +261,7 @@ !> \ingroup RRTMG -!! \defgroup module_radsw_main module_radsw_main +!! \defgroup module_radsw_main GFS RADSW Main !! This module includes NCEP's modifications of the rrtmg-sw radiation !! code from AER. !! diff --git a/physics/radsw_param.f b/physics/radsw_param.f index a1551395e..f2588cb18 100644 --- a/physics/radsw_param.f +++ b/physics/radsw_param.f @@ -1,7 +1,7 @@ !> \file radsw_param.f !! This file contains SW band parameters setup. -!> \ingroup module_radsw_main +!> \ingroup module_radsw_main !! @{ !!!!! ============================================================== !!!!! From 8ea46999e04285b7b8517ccabbd8a4c9bdf2dc3f Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Fri, 19 Jan 2018 16:56:50 -0700 Subject: [PATCH 02/22] add SAMF and part of SAMF_shal documentation --- physics/GFS_calpreciptype.f90 | 5 + physics/GFS_radupdate.f90 | 10 +- physics/docs/ccpp_dox | 11 - physics/docs/txt/mainpage.txt | 6 +- physics/mfdeepcnv.f | 758 +++++++++++++++++++++++++--------- physics/mfshalcnv.f | 62 ++- physics/radlw_main.f | 90 ++++ physics/sfc_diff.f | 4 +- physics/sfc_drv.f | 27 +- 9 files changed, 741 insertions(+), 232 deletions(-) diff --git a/physics/GFS_calpreciptype.f90 b/physics/GFS_calpreciptype.f90 index 7e0319cb6..17ecf30c7 100644 --- a/physics/GFS_calpreciptype.f90 +++ b/physics/GFS_calpreciptype.f90 @@ -2,6 +2,9 @@ !! This file contains the subroutine that calculates dominant precipitation type (calpreciptype) !! and its post. It is adopted from post but was made into a column to used by GFS model. +!>\defgroup CALPRECIPTYPE GFS Dominant Precipitation Type +!! @{ + module GFS_calpreciptype contains @@ -1519,3 +1522,5 @@ subroutine GFS_calpreciptype_finalize end subroutine GFS_calpreciptype_finalize end module GFS_calpreciptype + +!! @} diff --git a/physics/GFS_radupdate.f90 b/physics/GFS_radupdate.f90 index fe9349a55..e40732ffe 100644 --- a/physics/GFS_radupdate.f90 +++ b/physics/GFS_radupdate.f90 @@ -1,8 +1,15 @@ !>\file GFS_radupdate.f90 -!! This file contains +!! This file calls many update subroutines to check and update radiation required but +!! time varying data sets and module variables. module GFS_radupdate contains +!>\defgroup GFS_radupdate_run RRTMG Update +!!\ingroup RRTMG +!>\brief This subroutine calls many update subroutines to check and update radiation +!! required but time varying data sets and module variables. +!>\section gen_radupdate General Algorithm +!> @{ subroutine GFS_radupdate_run ( idate,jdate,deltsw,deltim,lsswr, me, & & slag,sdec,cdec,solcon, ictmflg, isolar) @@ -172,5 +179,6 @@ subroutine GFS_radupdate_run ( idate,jdate,deltsw,deltim,lsswr, me, & !................................... end subroutine GFS_radupdate_run !----------------------------------- +!> @} end module GFS_radupdate diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index c594a57c2..53cdc1445 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -112,16 +112,7 @@ INPUT = txt/mainpage.txt \ ../radsw_datatb.f \ ../radsw_main.f \ ../radsw_param.f \ -### Radiation interstitial - ../GFS_RRTMG_pre.f90 \ - ../GFS_RRTMG_post.f90 \ ../GFS_radupdate.f90 \ - ../GFS_rad_time_vary.f90 \ - ../GFS_radsw_pre.f90 \ - ../GFS_radsw_post.f90 \ - ../GFS_radlw_pre.f90 \ - ../GFS_radlw_post.f90 \ - ../radcons.f90 \ ### Deep Convection ../mfdeepcnv.f \ ### Shallow Convection @@ -132,8 +123,6 @@ INPUT = txt/mainpage.txt \ ### Microphysics ../precpd.f \ ../gscond.f \ -### MP_generic - ../GFS_MP_generic_post.f90 \ ../GFS_calpreciptype.f90 \ ### Land Surface ../sfc_drv.f \ diff --git a/physics/docs/txt/mainpage.txt b/physics/docs/txt/mainpage.txt index 4ef07b8b1..6410a3b3a 100644 --- a/physics/docs/txt/mainpage.txt +++ b/physics/docs/txt/mainpage.txt @@ -3,14 +3,16 @@ The documentation found here corresponds to the state of the operational GFS physics suite as of 2017. Documentation for the operational physics suite can be access through these links:: - \ref RRTMG - - \ref SASAS - - \ref SASHAL + - \ref SAMF + - \ref SAMF_shal - \ref HEDMF - \ref Zhao-Carr - \ref NOAH + - \ref Sfc_ex_cal - \ref GFS_Ice - \ref GFS_NSST - \ref GFS_ogwd - \ref GFS_cgwd - \ref GFS_ozn + - \ref CALPRECIPTYPE */ diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 4b812ddd6..bf293e24d 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -1,36 +1,118 @@ !> \file mfdeepcnv.f -!! This file contains NCEP's Scale Aware Simplified Arakawa Schubert Scheme -!! for deep convection. +!! This file contains the entire SAMF deep convection scheme. +!> \defgroup SAMF Scale-Aware Mass-Flux Deep Convection +!! @{ +!> \brief The scale-aware mass-flux (SAMF) deep convection scheme is an +!! updated version of the previous Simplified Arakawa-Schubert (SAS) scheme +!! with scale and aerosol awareness and parameterizes the effect of deep +!! convection on the environment (represented by the model state variables) +!! in the following way. First, a simple cloud model is used to determine +!! the change in model state variables due to one entraining/detraining cloud +!! type, per unit cloud-base mass flux. Next, the total change in state variables +!! is retrieved by determining the actual cloud base mass flux using the +!! quasi-equilibrium assumption (for grid sizes larger than a threshold value +!! [currently set to 8 km]) or a mean updraft velocity (for grid sizes smaller +!! than the threshold value). With a scale-aware parameterization, the +!! cloud mass flux decreases with increasing grid resolution. A simple +!! aerosol-aware parameterization is employed, where rain conversion in +!! the convective updraft is modified by aerosol number concentration. +!! The name SAS is replaced with SAMF as for the smaller grid sizes, +!! the parameterization does not use Arakawa-Schubert's quasi-equilibrium +!! assumption any longer where the cloud work function (interpreted as +!! entrainment-moderated convective available potential energy [CAPE]) +!! by the large scale dynamics is in balance with the consumption of the +!! cloud work function by the convection. +!! +!! The SAS scheme uses the working concepts put forth in Arakawa and +!! Schubert (1974) \cite arakawa_and_schubert_1974 but includes modifications +!! and simplifications from Grell (1993) \cite grell_1993 such as saturated +!! downdrafts and only one cloud type (the deepest possible), rather than +!! a spectrum based on cloud top heights or assumed entrainment rates. +!! The scheme was implemented for the GFS in 1995 by Pan and Wu +!! \cite pan_and_wu_1995, with further modifications discussed in +!! Han and Pan (2011) \cite han_and_pan_2011 , including the calculation +!! of cloud top, a greater CFL-criterion-based maximum cloud base mass flux, +!! updated cloud model entrainment and detrainment, improved convective +!! transport of horizontal momentum, a more general triggering function, +!! and the inclusion of convective overshooting. +!! +!! The SAMF scheme updates the SAS scheme with scale- and aerosol-aware +!! parameterizations from Han et al. (2017) \cite han_et_al_2017 based on +!! the studies by Arakawa and Wu (2013) \cite arakawa_and_wu_2013 and +!! Grell and Freitas (2014) \cite grell_and_freitas_2014 for scale awareness +!! and by Lim (2011) \cite lim_2011 for aerosol awareness. The ratio of +!! advective time to convective turnover time is also taken into account +!! for the scale-aware parameterization. Along with the scale- and aerosol-aware +!! parameterizations, more changes are made to the SAMF scheme. The cloud +!! base mass-flux computation is modified to use convective turnover time +!! as the convective adjustment time scale. The rain conversion rate is +!! modified to decrease with decreasing air temperature above the freezing +!! level. Convective inhibition in the sub-cloud layer is used as an additional +!! trigger condition. Convective cloudiness is enhanced by considering suspended +!! cloud condensate in the updraft. The lateral entrainment is also enhanced +!! to more strongly suppress convection in a drier environment. +!! +!! \section diagram Calling Hierarchy Diagram +!! \image html SAMF_Flowchart.png "Diagram depicting how the SAMF deep convection +!! scheme is called from the FV3GFS physics time loop" height=2cm +!! \section intraphysics Intraphysics Communication +!! This space is reserved for a description of how this scheme uses information +!! from other scheme types and/or how information calculated in this scheme +!! is used in other scheme types. + module sasas_deep contains -!> \defgroup SASAS Scale-Aware Simplified Arakawa-Schubert Deep Convection -!! @{ + !! \brief Brief description of the parameterization !! \section diagram Calling Hierarchy Diagram !! \section intraphysics Intraphysics Communication !> \brief Brief description of the subroutine !! -!! \section arg_table_sasasdeep_init Argument Table -!! | local var name | longname | description | units | rank | type | kind | intent | optional | -!! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| -!! +! \section arg_table_sasasdeep_init Argument Table +! | local var name | longname | description | units | rank | type | kind | intent | optional | +! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| +! subroutine sasasdeep_init end subroutine sasasdeep_init !> \brief Brief description of the subroutine !! -!! \section arg_table_sasasdeep_finalize Argument Table -!! | local var name | longname | description | units | rank | type | kind | intent | optional | -!! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| -!! +! \section arg_table_sasasdeep_finalize Argument Table +! | local var name | longname | description | units | rank | type | kind | intent | optional | +! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| +! subroutine sasasdeep_finalize end subroutine sasasdeep_finalize -!> \brief Brief description of the subroutine + +!>\brief This subroutine contains the entirety of the SAMF deep convection scheme. +!! +!! For grid sizes larger than threshold value, as in Grell (1993) +!! \cite grell_1993 , the SAMF deep convection scheme can be described +!! in terms of three types of "controls": static, dynamic, and feedback. +!! The static control component consists of the simple entraining/detraining +!! updraft/downdraft cloud model and is used to determine the cloud +!! properties, convective precipitation, as well as the convective cloud +!! top height. The dynamic control is the determination of the potential +!! energy available for convection to "consume", or how primed the +!! large-scale environment is for convection to occur due to changes by +!! the dyanmics of the host model. The feedback control is the +!! determination of how the parameterized convection changes the +!! large-scale environment (the host model state variables) given the +!! changes to the state variables per unit cloud base mass flux calculated +!! in the static control portion and the deduced cloud base mass flux +!! determined from the dynamic control. +!! +!! For grid sizes smaller than threshold value, the cloud base mass flux +!! in the SAMF scheme is determined by the cumulus updraft velocity averaged +!! over the whole cloud depth (Han et al., 2017 \cite han_et_al_2017 ), which +!! in turn, determines changes of the large-scale environment due to the +!! cumulus convection. +!! !! !! \section arg_table_sasasdeep_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -65,6 +147,34 @@ end subroutine sasasdeep_finalize !! | cnvc | convective_cloud_cover | convective cloud cover | frac | 2 | real | kind_phys | out | F | !! !! \section general General Algorithm +!! -# Compute preliminary quantities needed for static, dynamic, and +!! feedback control portions of the algorithm. +!! -# Perform calculations related to the updraft of the entraining/detraining +!! cloud model ("static control"). +!! -# Perform calculations related to the downdraft of the entraining/detraining +!! cloud model ("static control"). +!! +!! -# For grid sizes larger than the threshold value (currently 8 km): +!! - 1) Using the updated temperature and moisture profiles that were +!! modified by the convection on a short time-scale, recalculate the +!! total cloud work function to determine the change in the cloud work +!! function due to convection, or the stabilizing effect of the cumulus. +!! - 2) For the "dynamic control", using a reference cloud work function, +!! estimate the change in cloud work function due to the large-scale dynamics. +!! Following the quasi-equilibrium assumption, calculate the cloud base +!! mass flux required to keep the large-scale convective destabilization +!! in balance with the stabilization effect of the convection. +!! +!! -# For grid sizes smaller than the threshold value (currently 8 km): +!! - 1) compute the cloud base mass flux using the cumulus updraft +!! velocity averaged ove the whole cloud depth. +!! +!! -# For scale awareness, the updraft fraction (sigma) is obtained as +!! a function of cloud base entrainment. Then, the final cloud base mass +!! flux is obtained by the original mass flux multiplied by the \f$(1-sigma)^2\f$. +!! -# For the "feedback control", calculate updated values of the state +!! variables by multiplying the cloud base mass flux and the tendencies +!! calculated per unit cloud base mass flux from the static control. !! \section detailed Detailed Algorithm !! @{ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & @@ -175,12 +285,12 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & parameter(c0s=.002,c1=.002,d0=.01) parameter(c0l=c0s*asolfac) -!> asolfac: aerosol-aware parameter based on Lim & Hong (2012) -!! asolfac= cx / c0s(=.002) -!! cx = min([-0.7 ln(Nccn) + 24]*1.e-4, c0s) -!! Nccn: CCN number concentration in cm^(-3) -!! Until a realistic Nccn is provided, typical Nccns are assumed -!! as Nccn=100 for sea and Nccn=7000 for land +! asolfac: aerosol-aware parameter based on Lim & Hong (2012) +! asolfac= cx / c0s(=.002) +! cx = min([-0.7 ln(Nccn) + 24]*1.e-4, c0s) +! Nccn: CCN number concentration in cm^(-3) +! Until a realistic Nccn is provided, typical Nccns are assumed +! as Nccn=100 for sea and Nccn=7000 for land parameter(cm=1.0,delta=fv) parameter(fact1=(cvap-cliq)/rv,fact2=hvap/rv-fact1*t0c) @@ -191,14 +301,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & parameter(bet1=1.875,cd1=.506,f1=2.0,gam1=.5) parameter(betaw=.03,dxcrtas=8.e3,dxcrtuf=15.e3) -!> local variables and arrays +! local variables and arrays real(kind=kind_phys) pfld(im,km), to(im,km), qo(im,km), & uo(im,km), vo(im,km), qeso(im,km) -!> for updraft velocity calculation +! for updraft velocity calculation real(kind=kind_phys) wu2(im,km), buo(im,km), drag(im,km) real(kind=kind_phys) wc(im), scaldfunc(im), sigmagfm(im) -!> cloud water +! cloud water ! real(kind=kind_phys) tvo(im,km) real(kind=kind_phys) qlko_ktcon(im), dellal(im,km), tvo(im,km), & dbyo(im,km), zo(im,km), @@ -216,7 +326,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & logical totflg, cnvflg(im), asqecflg(im), flg(im) -!> asqecflg: flag for the quasi-equilibrium assumption of Arakawa-Schubert +! asqecflg: flag for the quasi-equilibrium assumption of Arakawa-Schubert ! real(kind=kind_phys) pcrit(15), acritt(15), acrit(15) !! save pcrit, acritt @@ -231,7 +341,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & parameter (tf=233.16, tcr=263.16, tcrf=1.0/(tcr-tf)) ! c----------------------------------------------------------------------- -! +!> ## Compute preliminary quantities needed for static, dynamic, and feedback control portions of the algorithm. +!> - Convert input pressure terms to centibar units. !************************************************************************ !> convert input Pa terms to Cb terms -- Moorthi ps = psp * 0.001 @@ -241,9 +352,10 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! ! km1 = km - 1 - -!> initialize arrays - +!> - Initialize column-integrated and other single-value-per-column variable arrays. +c +c initialize arrays +c do i=1,im cnvflg(i) = .true. rn(i)=0. @@ -276,6 +388,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & gdx(i) = sqrt(garea(i)) enddo ! +!> - determine aerosol-aware rain conversion parameter over land do i=1,im if(islimsk(i) == 1) then c0(i) = c0l @@ -283,6 +396,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c0(i) = c0s endif enddo +!> - determine rain conversion parameter above the freezing level which +!! exponentially decreases with decreasing temperature from Han et al.'s (2017) +!! \cite han_et_al_2017 equation 8. do k = 1, km do i = 1, im if(t1(i,k) > 273.16) then @@ -294,7 +410,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo -! +!> - Initialize convective cloud water and cloud cover to zero. do k = 1, km do i = 1, im cnvw(i,k) = 0. @@ -302,6 +418,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo ! hchuang code change +!> - Initialize updraft and downdraft mass fluxes to zero. do k = 1, km do i = 1, im ud_mf(i,k) = 0. @@ -321,7 +438,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! val = 5400. val = 10800. dtmax = max(dt2, val ) -!> model tunable parameters are all here +c model tunable parameters are all here edtmaxl = .3 edtmaxs = .3 clam = .1 @@ -353,10 +470,12 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & w2s = -2.e-3 w3s = -1.e-3 w4s = -2.e-5 - -!> define top layer for search of the downdraft originating layer -!! and the maximum thetae for updraft - +c +c define top layer for search of the downdraft originating layer +c and the maximum thetae for updraft +c +!> - Determine maximum indices for the parcel starting point (kbm), +!! LFC (kbmax), and cloud top (kmax). do i=1,im kbmax(i) = km kbm(i) = km @@ -376,16 +495,17 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & kbmax(i) = min(kbmax(i),kmax(i)) kbm(i) = min(kbm(i),kmax(i)) enddo - -!> hydrostatic height assume zero terr and initially assume -!! updraft entrainment rate as an inverse function of height - - +c +c hydrostatic height assume zero terr and initially assume +c updraft entrainment rate as an inverse function of height +c +!> - Calculate hydrostatic height at layer centers assuming a flat surface (no terrain) from the geopotential. do k = 1, km do i=1,im zo(i,k) = phil(i,k) / g enddo enddo +!> - Calculate interface height and the initial entrainment rate as an inverse function of height. do k = 1, km1 do i=1,im zi(i,k) = 0.5*(zo(i,k)+zo(i,k+1)) @@ -393,9 +513,13 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! xlamue(i,k) = max(xlamue(i,k), crtlamu) enddo enddo - -!> convert surface pressure to mb from cb - +c +c!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! +c convert surface pressure to mb from cb +c +!> - Convert prsl from centibar to millibar, set normalized mass fluxes +!! to 1, cloud properties to 0, and save model state variables (after +!! advection/turbulence). do k = 1, km do i = 1, im if (k <= kmax(i)) then @@ -433,14 +557,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> column variables -!! p is pressure of the layer (mb) -!! t is temperature at t-dt (k)..tn -!! q is specific humidity at t-dt (kg/kg)..qn -!! to is temperature at t+dt (k)... this is after advection and turbulence -!! qo is specific humidity at t+dt (kg/kg)..q1 - +!> - Calculate saturation specific humidity and enforce minimum moisture values. do k = 1, km do i=1,im if (k <= kmax(i)) then @@ -455,9 +572,10 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> compute moist static energy - +c +c compute moist static energy +c +!> - Calculate moist static energy (heo) and saturation moist static energy (heso). do k = 1, km do i=1,im if (k <= kmax(i)) then @@ -469,10 +587,12 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> determine level with largest moist static energy -!! this is the level where updraft starts - +c +c determine level with largest moist static energy +c this is the level where updraft starts +c +!> ## Perform calculations related to the updraft of the entraining/detraining cloud model ("static control"). +!> - Search below index "kbm" for the level of maximum moist static energy. do i=1,im hmax(i) = heo(i,1) kb(i) = 1 @@ -488,6 +608,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo c +!> - Calculate the temperature, specific humidity, and pressure at interface levels. do k = 1, km1 do i=1,im if (k <= kmax(i)-1) then @@ -509,6 +630,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo ! +!> - Recalculate saturation specific humidity, moist static energy, saturation +!! moist static energy, and horizontal momentum on interface levels. Enforce +!! minimum specific humidity and calculate \f$(1 - RH)\f$. do k = 1, km1 do i=1,im if (k <= kmax(i)-1) then @@ -529,9 +653,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> look for the level of free convection as cloud base - +c +c look for the level of free convection as cloud base +c +!> - Search below the index "kbmax" for the level of free convection (LFC) +!! where the condition \f$h_b > h^*\f$ is first met, where \f$h_b, h^*\f$ +!! are the state moist static energy at the parcel's starting level and +!! saturation moist static energy, respectively. Set "kbcon" to the index +!! of the LFC. do i=1,im flg(i) = .true. kbcon(i) = kmax(i) @@ -547,6 +676,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo c +!> - If no LFC, return to the calling routine without modifying state variables. do i=1,im if(kbcon(i) == kmax(i)) cnvflg(i) = .false. enddo @@ -557,16 +687,23 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo if(totflg) return !! +!> - Determine the vertical pressure velocity at the LFC. After Han and +!! Pan (2011) \cite han_and_pan_2011 , determine the maximum pressure +!! thickness between a parcel's starting level and the LFC. If a parcel +!! doesn't reach the LFC within the critical thickness, then the +!! convective inhibition is deemed too great for convection to be +!! triggered, and the subroutine returns to the calling routine without +!! modifying the state variables. do i=1,im if(cnvflg(i)) then ! pdot(i) = 10.* dot(i,kbcon(i)) pdot(i) = 0.01 * dot(i,kbcon(i)) ! Now dot is in Pa/s endif enddo - -!> turn off convection if pressure depth between parcel source level -!! and cloud base is larger than a critical value, cinpcr - +c +c turn off convection if pressure depth between parcel source level +c and cloud base is larger than a critical value, cinpcr +c do i=1,im if(cnvflg(i)) then if(islimsk(i) == 1) then @@ -606,10 +743,23 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & totflg = totflg .and. (.not. cnvflg(i)) enddo if(totflg) return - -!> assume that updraft entrainment rate above cloud base is -!! same as that at cloud base - +!! +c +c assume that updraft entrainment rate above cloud base is +c same as that at cloud base +c +!> - Calculate the entrainment rate according to Han and Pan (2011) +!! \cite han_and_pan_2011, equation 8, after Bechtold et al. (2008) +!! \cite bechtold_et_al_2008, equation 2 given by: +!! \f[ +!! \epsilon = \epsilon_0F_0 + d_1\left(1-RH\right)F_1 +!! \f] +!! where \f$\epsilon_0\f$ is the cloud base entrainment rate, \f$d_1\f$ +!! is a tunable constant, and \f$F_0=\left(\frac{q_s}{q_{s,b}}\right)^2\f$ and +!! \f$F_1=\left(\frac{q_s}{q_{s,b}}\right)^3\f$ where \f$q_s\f$ and +!! \f$q_{s,b}\f$ are the saturation specific humidities at a given level +!! and cloud base, respectively. The detrainment rate in the cloud is +!! assumed to be equal to the entrainment rate at cloud base. do i=1,im if(cnvflg(i)) then xlamx(i) = xlamue(i,kbcon(i)) @@ -623,9 +773,11 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> specify a background (turbulent) detrainment rate for the updrafts - +c +c specify a background (turbulent) detrainment rate for the updrafts +c +!> - The updraft detrainment rate is set constant and equal to the +!! entrainment rate at cloud base. do k = 1, km1 do i=1,im if(cnvflg(i) .and. k < kmax(i)) then @@ -634,9 +786,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> functions rapidly decreasing with height, mimicking a cloud ensemble -!! (Bechtold et al., 2008) +c +c functions rapidly decreasing with height, mimicking a cloud ensemble +c (Bechtold et al., 2008) do k = 2, km1 do i=1,im @@ -648,11 +800,11 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> final entrainment and detrainment rates as the sum of turbulent part and -!! organized entrainment depending on the environmental relative humidity -!! (Bechtold et al., 2008) - +c +c final entrainment and detrainment rates as the sum of turbulent part and +c organized entrainment depending on the environmental relative humidity +c (Bechtold et al., 2008) +c do k = 2, km1 do i=1,im if(cnvflg(i) .and. @@ -664,9 +816,18 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> determine updraft mass flux for the subcloud layers - +! +!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! +c +c determine updraft mass flux for the subcloud layers +c +!> - Calculate the normalized mass flux for subcloud and in-cloud layers +!! according to Pan and Wu (1995) \cite pan_and_wu_1995 equation 1: +!! \f[ +!! \frac{1}{\eta}\frac{\partial \eta}{\partial z} = \lambda_e - \lambda_d +!! \f] +!! where \f$\eta\f$ is the normalized mass flux, \f$\lambda_e\f$ is the +!! entrainment rate and \f$\lambda_d\f$ is the detrainment rate. do k = km1, 1, -1 do i = 1, im if (cnvflg(i)) then @@ -679,9 +840,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> compute mass flux above cloud base - +c +c compute mass flux above cloud base +c do i = 1, im flg(i) = cnvflg(i) enddo @@ -702,9 +863,10 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> compute updraft cloud properties - +c +c compute updraft cloud properties +c +!> - Set cloud properties equal to the state variables at updraft starting level (kb). do i = 1, im if(cnvflg(i)) then indx = kb(i) @@ -714,11 +876,18 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & pwavo(i) = 0. endif enddo - -!> cloud property is modified by the entrainment process - -!> cm is an enhancement factor in entrainment rates for momentum - +c +c cloud property is modified by the entrainment process +c +! cm is an enhancement factor in entrainment rates for momentum +! +!> - Calculate the cloud properties as a parcel ascends, modified by +!! entrainment and detrainment. Discretization follows Appendix B of +!! Grell (1993) \cite grell_1993 . Following Han and Pan (2006) +!! \cite han_and_pan_2006, the convective momentum transport is reduced +!! by the convection-induced pressure gradient force by the constant +!! "pgcon", currently set to 0.55 after Zhang and Wu (2003) +!! \cite zhang_and_wu_2003 . do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -743,10 +912,17 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> taking account into convection inhibition due to existence of -!! dry layers below cloud base - +c +c taking account into convection inhibition due to existence of +c dry layers below cloud base +c +!> - With entrainment, recalculate the LFC as the first level where +!! buoyancy is positive. The difference in pressure levels between LFCs +!! calculated with/without entrainment must be less than a threshold +!! (currently 25 hPa). Otherwise, convection is inhibited and the scheme +!! returns to the calling routine without modifying the state variables. +!! This is the subcloud dryness trigger modification discussed in Han +!! and Pan (2011) \cite han_and_pan_2011. do i=1,im flg(i) = cnvflg(i) kbcon1(i) = kmax(i) @@ -781,9 +957,11 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo if(totflg) return !! - -!> calculate convective inhibition - +c +c calculate convective inhibition +c +!> - Calculate additional trigger condition of the convective inhibition +!! (CIN) according to Han et al.'s (2017) \cite han_et_al_2017 equation 13. do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -806,6 +984,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo +!> - Turn off convection if the CIN is less than a critical value +!! (cinacr) which is inversely proportional to the large-scale vertical velocity. do i = 1, im if(cnvflg(i)) then ! @@ -846,9 +1026,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & totflg = totflg .and. (.not. cnvflg(i)) enddo if(totflg) return - -!> determine first guess cloud top as the level of zero buoyancy - +!! +c +c determine first guess cloud top as the level of zero buoyancy +c +!> - Calculate the cloud top as the first level where parcel buoyancy +!! becomes negative. If the thickness of the calculated convection is +!! less than a threshold (currently 200 hPa), then convection is +!! inhibited, and the scheme returns to the calling routine. do i = 1, im flg(i) = cnvflg(i) ktcon(i) = 1 @@ -879,9 +1064,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & totflg = totflg .and. (.not. cnvflg(i)) enddo if(totflg) return - -!> search for downdraft originating level above theta-e minimum - +!! +c +c search for downdraft originating level above theta-e minimum +c +!> - To originate the downdraft, search for the level above the minimum +!! in moist static energy. Return to the calling routine without +!! modification if this level is determined to be outside of the +!! convective cloud layers. do i = 1, im if(cnvflg(i)) then hmin(i) = heo(i,kbcon1(i)) @@ -899,9 +1089,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> make sure that jmin(i) is within the cloud - +c +c make sure that jmin(i) is within the cloud +c do i = 1, im if(cnvflg(i)) then jmin(i) = min(lmin(i),ktcon(i)-1) @@ -909,9 +1099,12 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & if(jmin(i) >= ktcon(i)) cnvflg(i) = .false. endif enddo - -!> specify upper limit of mass flux at cloud base - +c +c specify upper limit of mass flux at cloud base +c +!> - Calculate the maximum value of the cloud base mass flux using the +!! CFL-criterion-based formula of Han and Pan (2011) \cite han_and_pan_2011, +!! equation 7. do i = 1, im if(cnvflg(i)) then ! xmbmax(i) = .1 @@ -926,9 +1119,11 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! xmbmax(i) = min(tem, xmbmax(i)) endif enddo - -!> compute cloud moisture property and precipitation - +c +c compute cloud moisture property and precipitation +c +!> - Set cloud moisture property equal to the enviromental moisture at +!! updraft starting level (kb). do i = 1, im if (cnvflg(i)) then ! aa1(i) = 0. @@ -937,6 +1132,16 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! rhbar(i) = 0. endif enddo +!> - Calculate the moisture content of the entraining/detraining parcel +!! (qcko) and the value it would have if just saturated (qrch), according +!! to equation A.14 in Grell (1993) \cite grell_1993 . Their difference +!! is the amount of convective cloud water (qlk = rain + condensate). +!! Determine the portion of convective cloud water that remains suspended +!! and the portion that is converted into convective precipitation (pwo). +!! Calculate and save the negative cloud work function (aa1) due to water +!! loading. The liquid water in the updraft layer is assumed to be detrained +!! from the layers above the level of the minimum moist static energy into +!! the grid-scale cloud water (dellal). do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -956,9 +1161,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & dq = eta(i,k) * (qcko(i,k) - qrch) c ! rhbar(i) = rhbar(i) + qo(i,k) / qeso(i,k) - -!> check if there is excess moisture to release latent heat - +c +c check if there is excess moisture to release latent heat +c if(k >= kbcon(i) .and. dq > 0.) then etah = .5 * (eta(i,k) + eta(i,k-1)) if(ncloud > 0 .and. k > jmin(i)) then @@ -978,9 +1183,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! cnvwt(i,k) = (etah*qlk + pwo(i,k)) * g / dp cnvwt(i,k) = etah * qlk * g / dp endif - -!> compute buoyancy and drag for updraft velocity - +! +! compute buoyancy and drag for updraft velocity +! if(k >= kbcon(i)) then rfact = 1. + delta * cp * gamma & * to(i,k) / hvap @@ -1004,9 +1209,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! rhbar(i) = rhbar(i) / float(indx) ! endif ! enddo - -!> calculate cloud work function - +c +c calculate cloud work function +c ! do k = 2, km1 ! do i = 1, im ! if (cnvflg(i)) then @@ -1030,8 +1235,19 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! enddo ! enddo -!> calculate cloud work function - +! calculate cloud work function +!> - Calculate the cloud work function according to Pan and Wu (1995) +!! \cite pan_and_wu_1995 equation 4: +!! \f[ +!! A_u=\int_{z_0}^{z_t}\frac{g}{c_pT(z)}\frac{\eta}{1 + \gamma}[h(z)-h^*(z)]dz +!! \f] +!! (discretized according to Grell (1993) \cite grell_1993 equation B.10 +!! using B.2 and B.3 of Arakawa and Schubert (1974) \cite arakawa_and_schubert_1974 +!! and assuming \f$\eta=1\f$) where \f$A_u\f$ is the updraft cloud work +!! function, \f$z_0\f$ and \f$z_t\f$ are cloud base and cloud top, +!! respectively, \f$\gamma = \frac{L}{c_p}\left(\frac{\partial \overline{q_s}}{\partial T}\right)_p\f$ +!! and other quantities are previously defined. + do i = 1, im do i = 1, im if (cnvflg(i)) then aa1(i) = 0. @@ -1049,6 +1265,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo ! +!> - If the updraft cloud work function is negative, convection does not +!! occur, and the scheme returns to the calling routine. do i = 1, im if(cnvflg(i) .and. aa1(i) <= 0.) cnvflg(i) = .false. enddo @@ -1058,11 +1276,17 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & totflg = totflg .and. (.not. cnvflg(i)) enddo if(totflg) return - -!> estimate the onvective overshooting as the level -!! where the [aafac * cloud work function] becomes zero, -!! which is the final cloud top - +!! +c +c estimate the onvective overshooting as the level +c where the [aafac * cloud work function] becomes zero, +c which is the final cloud top +c +!> - Continue calculating the cloud work function past the point of +!! neutral buoyancy to represent overshooting according to Han and Pan +!! (2011) \cite han_and_pan_2011 . Convective overshooting stops when +!! \f$ cA_u < 0\f$ where \f$c\f$ is currently 10%, or when 10% of the +!! updraft cloud work function has been consumed by the stable buoyancy force. do i = 1, im if (cnvflg(i)) then aa2(i) = aafac * aa1(i) @@ -1099,10 +1323,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> compute cloud moisture property, detraining cloud water -!! and precipitation in overshooting layers - +c +c compute cloud moisture property, detraining cloud water +c and precipitation in overshooting layers +c +!> - For the overshooting convection, calculate the moisture content of +!! the entraining/detraining parcel as before. Partition convective +!! cloud water and precipitation and detrain convective cloud water +!! above the mimimum in moist static energy. do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -1120,9 +1348,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & qrcko(i,k) = qcko(i,k) cj dq = eta(i,k) * (qcko(i,k) - qrch) - -!> check if there is excess moisture to release latent heat - +c +c check if there is excess moisture to release latent heat +c if(dq > 0.) then etah = .5 * (eta(i,k) + eta(i,k-1)) if(ncloud > 0) then @@ -1143,9 +1371,10 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> compute updraft velocity square(wu2) - +! +! compute updraft velocity square(wu2) +!> - Calculate updraft velocity square(wu2) according to Han et al.'s +!! (2017) \cite han_et_al_2017 equation 7. ! bb1 = 2. * (1.+bet1*cd1) ! bb2 = 2. / (f1*(1.+gam1)) ! @@ -1185,9 +1414,10 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> compute updraft velocity average over the whole cumulus - +! +! compute updraft velocity average over the whole cumulus +! +!> - Calculate the mean updraft velocity within the cloud (wc). do i = 1, im wc(i) = 0. sumx(i) = 0. @@ -1215,9 +1445,12 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & if (wc(i) < val) cnvflg(i)=.false. endif enddo - -!> exchange ktcon with ktcon1 - +c +c exchange ktcon with ktcon1 +c +!> - Swap the indices of the convective cloud top (ktcon) and the +!! overshooting convection top (ktcon1) to use the same cloud top level +!! in the calculations of \f$A^+\f$ and \f$A^*\f$. do i = 1, im if(cnvflg(i)) then kk = ktcon(i) @@ -1225,13 +1458,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ktcon1(i) = kk endif enddo - -!> this section is ready for cloud water - +c +c this section is ready for cloud water +c +!> - Separate the total updraft cloud water at cloud top into vapor and condensate. if(ncloud > 0) then - -!> compute liquid and vapor separation at cloud top - +c +c compute liquid and vapor separation at cloud top +c do i = 1, im if(cnvflg(i)) then k = ktcon(i) - 1 @@ -1239,9 +1473,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & qrch = qeso(i,k) & + gamma * dbyo(i,k) / (hvap * (1. + gamma)) dq = qcko(i,k) - qrch - -!> check if there is excess moisture to release latent heat - +c +c check if there is excess moisture to release latent heat +c if(dq > 0.) then qlko_ktcon(i) = dq qcko(i,k) = qrch @@ -1253,10 +1487,24 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ccccc if(lat.==.latd.and.lon.==.lond.and.cnvflg(i)) then ccccc print *, ' aa1(i) before dwndrft =', aa1(i) ccccc endif - -!> ----- downdraft calculations - -!> - compute precipitation efficiency in terms of windshear +c +c ----- downdraft calculations +c +c - compute precipitation efficiency in terms of windshear +c +!> ## Perform calculations related to the downdraft of the entraining/detraining +!! cloud model ("static control"). +!! - First, in order to calculate the downdraft mass flux (as a fraction +!! of the updraft mass flux), calculate the wind shear and precipitation +!! efficiency according to equation 58 in Fritsch and Chappell (1980) +!! \cite fritsch_and_chappell_1980 : +!! \f[ +!! E = 1.591 - 0.639\frac{\Delta V}{\Delta z} + 0.0953\left(\frac{\Delta V}{\Delta z}\right)^2 - 0.00496\left(\frac{\Delta V}{\Delta z}\right)^3 +!! \f] +!! where \f$\Delta V\f$ is the integrated horizontal shear over the +!! cloud depth, \f$\Delta z\f$, (the ratio is converted to units of +!! \f$10^{-3} s^{-1}\f$). The variable "edto" is \f$1-E\f$ and is +!! constrained to the range \f$[0,0.9]\f$. do i = 1, im if(cnvflg(i)) then @@ -1288,9 +1536,19 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & edtx(i)=edt(i) endif enddo - -!> determine detrainment rate between 1 and kbcon - +c +c determine detrainment rate between 1 and kbcon +c +!> - Next, calculate the variable detrainment rate between the surface +!! and the LFC according to: +!! \f[ +!! \lambda_d = \frac{1-\beta^{\frac{1}{k_{LFC}}}}{\overline{\Delta z}} +!! \f] +!! \f$\lambda_d\f$ is the detrainment rate, \f$\beta\f$ is a constant +!! currently set to 0.05, implying that only 5% of downdraft mass flux +!! at LFC reaches the ground surface due to detrainment, \f$k_{LFC}\f$ +!! is the vertical index of the LFC level, and \f$\overline{\Delta z}\f$ +!! is the average vertical grid spacing below the LFC. do i = 1, im if(cnvflg(i)) then sumx(i) = 0. @@ -1315,9 +1573,13 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & xlamd(i) = (1.-beta**tem)/dz endif enddo - -!> determine downdraft mass flux - +c +c determine downdraft mass flux +c +!> - Calculate the normalized downdraft mass flux from equation 1 of Pan +!! and Wu (1995) \cite pan_and_wu_1995 . Downdraft entrainment and +!! detrainment rates are constants from the downdraft origination to +!! the LFC. do k = km1, 1, -1 do i = 1, im if (cnvflg(i) .and. k <= kmax(i)-1) then @@ -1333,9 +1595,11 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> - downdraft moisture properties - +c +c--- downdraft moisture properties +c +!> - Set initial cloud downdraft properties equal to the state variables +!! at the downdraft origination level. do i = 1, im if(cnvflg(i)) then jmn = jmin(i) @@ -1348,6 +1612,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo cj +!> - Calculate the cloud properties as a parcel descends, modified by +!! entrainment and detrainment. Discretization follows Appendix B of +!! Grell (1993) \cite grell_1993 . do k = km1, 1, -1 do i = 1, im if (cnvflg(i) .and. k < jmin(i)) then @@ -1376,6 +1643,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo c +!> - Compute the amount of moisture that is necessary to keep the downdraft +!! saturated. do k = km1, 1, -1 do i = 1, im if (cnvflg(i) .and. k < jmin(i)) then @@ -1406,11 +1675,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo - -!> - final downdraft strength dependent on precip -!! - efficiency (edt), normalized condensate (pwav), and -!! - evaporate (pwev) - +c +c--- final downdraft strength dependent on precip +c--- efficiency (edt), normalized condensate (pwav), and +c--- evaporate (pwev) +c +!> - Update the precipitation efficiency (edto) based on the ratio of +!! normalized cloud condensate (pwavo) to normalized cloud evaporate +!! (pwevo). do i = 1, im edtmax = edtmaxl if(islimsk(i) == 0) edtmax = edtmaxs @@ -1426,6 +1698,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c--- downdraft cloudwork functions c +!> - Calculate downdraft cloud work function (\f$A_d\f$) according to +!! equation A.42 (discretized by B.11) in Grell (1993) \cite grell_1993 . +!! Add it to the updraft cloud work function, \f$A_u\f$. do k = km1, 1, -1 do i = 1, im if (cnvflg(i) .and. k < jmin(i)) then @@ -1446,6 +1721,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo +!> - Check for negative total cloud work function; if found, return to +!! calling routine without modifying state variables. do i = 1, im if(cnvflg(i) .and. aa1(i) <= 0.) then cnvflg(i) = .false. @@ -1462,6 +1739,11 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c--- what would the change be, that a cloud with unit mass c--- will do to the environment? c +!> - Calculate the change in moist static energy, moisture mixing ratio, +!! and horizontal winds per unit cloud base mass flux near the surface +!! using equations B.18 and B.19 from Grell (1993) \cite grell_1993, for +!! all layers below cloud top from equations B.14 and B.15, and for the +!! cloud top from B.16 and B.17. do k = 1, km do i = 1, im if(cnvflg(i) .and. k <= kmax(i)) then @@ -1576,9 +1858,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c------- final changed variable per unit mass flux c -! if grid size is less than a threshold value (dxcrtas), -! the quasi-equilibrium assumption of Arakawa-Schubert is not -! used any longer. +!> - If grid size is less than a threshold value (dxcrtas: currently 8km), +!! the quasi-equilibrium assumption of Arakawa-Schubert is not used any longer. ! do i = 1, im asqecflg(i) = cnvflg(i) @@ -1587,6 +1868,10 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo ! +!> - If grid size is larger than the threshold value (i.e., asqecflg=.true.), +!! the quasi-equilibrium assumption is used to obtain the cloud base mass flux. +!! To begin with, calculate the change in the temperature and moisture +!! profiles per unit cloud base mass flux. do k = 1, km do i = 1, im if (asqecflg(i) .and. k <= kmax(i)) then @@ -1615,6 +1900,17 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c--- environmental conditions again, first heights c +!> ## Using the updated temperature and moisture profiles that were +!! modified by the convection on a short time-scale, recalculate the +!! total cloud work function to determine the change in the cloud work +!! function due to convection, or the stabilizing effect of the cumulus. +!! - Using notation from Pan and Wu (1995) \cite pan_and_wu_1995, the +!! previously calculated cloud work function is denoted by \f$A^+\f$. +!! Now, it is necessary to use the entraining/detraining cloud model +!! ("static control") to determine the cloud work function of the +!! environment after the stabilization of the arbitrary convective element +!! (per unit cloud base mass flux) has been applied, denoted by \f$A^*\f$. +!! - Recalculate saturation specific humidity. do k = 1, km do i = 1, im if(asqecflg(i) .and. k <= kmax(i)) then @@ -1629,6 +1925,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c--- moist static energy c +!! - Recalculate moist static energy and saturation moist static energy. do k = 1, km1 do i = 1, im if(asqecflg(i) .and. k <= kmax(i)-1) then @@ -1679,6 +1976,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c------- moisture and cloud work functions c +!> - As before, recalculate the updraft cloud work function. do i = 1, im if(asqecflg(i)) then xaa0(i) = 0. @@ -1766,6 +2064,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c--- downdraft moisture properties c +!> - As before, recalculate the downdraft cloud work function. do i = 1, im if(asqecflg(i)) then jmn = jmin(i) @@ -1933,6 +2232,11 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! ! compute convective turn-over time ! +!> - Following Bechtold et al. (2008) \cite bechtold_et_al_2008, the +!! convective adjustment time (dtconv) is set to be proportional to the +!! convective turnover time, which is computed using the mean updraft +!! velocity (wc) and the cloud depth. It is also proportional to the +!! grid size (gdx). do i= 1, im if(cnvflg(i)) then tem = zi(i,ktcon1(i)) - zi(i,kbcon1(i)) @@ -1944,8 +2248,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo ! -! compute advective time scale using a mean cloud layer wind speed -! +!> - Calculate advective time scale (tauadv) using a mean cloud layer wind speed. do i= 1, im if(cnvflg(i)) then sumx(i) = 0. @@ -1971,12 +2274,15 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & tauadv(i) = gdx(i) / umean(i) endif enddo -c -c compute cloud base mass flux as a function of the mean -c updraft velcoity for the grid sizes where -c the quasi-equilibrium assumption of Arakawa-Schubert is not -c valid any longer. -c +!> - From Han et al.'s (2017) \cite han_et_al_2017 equation 6, calculate +!! cloud base mass flux as a function of the mean updraft velcoity for +!! the grid sizes where the quasi-equilibrium assumption of Arakawa-Schubert +!! is not valid any longer. +!! As discussed in Han et al. (2017) \cite han_et_al_2017 , when dtconv +!! is larger than tauadv, the convective mixing is not fully conducted +!! before the cumulus cloud is advected out of the grid cell. In this case, +!! therefore, the cloud base mass flux is further reduced in proportion +!! to the ratio of tauadv to dtconv. do i= 1, im if(cnvflg(i) .and. .not.asqecflg(i)) then k = kbcon(i) @@ -1986,10 +2292,16 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & xmb(i) = tfac*betaw*rho*wc(i) endif enddo -c -c compute cloud base mass flux using -c the quasi-equilibrium assumption of Arakawa-Schubert -c +!> - For the cases where the quasi-equilibrium assumption of +!! Arakawa-Schubert is valid, first calculate the large scale +!! destabilization as in equation 5 of Pan and Wu (1995) +!! \cite pan_and_wu_1995 : +!! \f[ +!! \frac{\partial A}{\partial t}_{LS}=\frac{A^+-cA^0}{\Delta t_{LS}} +!! \f] +!! Here \f$A^0\f$ is set to zero following Han et al.'s (2017) +!! \cite han_et_al_2017 , implying that the instability is completely +!! eliminated after the convective adjustment time, \f$\Delta t_{LS}\f$. do i= 1, im if(asqecflg(i)) then ! fld(i)=(aa1(i)-acrt(i)*acrtfct(i))/dtconv(i) @@ -1999,6 +2311,13 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & cnvflg(i) = .false. endif endif +!> - Calculate the stabilization effect of the convection (per unit +!! cloud base mass flux) as in equation 6 of Pan and Wu (1995) +!! \cite pan_and_wu_1995 : +!! \f[ +!! \frac{\partial A}{\partial t}_{cu}=\frac{A^*-A^+}{\Delta t_{cu}} +!! \f] +!! \f$\Delta t_{cu}\f$ is the short timescale of the convection. if(asqecflg(i)) then c xaa0(i) = max(xaa0(i),0.) xk(i) = (xaa0(i) - aa1(i)) / mbdt(i) @@ -2010,6 +2329,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c--- kernel, cloud base mass flux c +!> - The cloud base mass flux (xmb) is then calculated from equation +!! 7 of Pan and Wu (1995) \cite pan_and_wu_1995 +!! \f[ +!! M_c=\frac{-\frac{\partial A}{\partial t}_{LS}}{\frac{\partial A}{\partial t}_{cu}} +!! \f] +!! +!! Again when dtconv is larger than tauadv, the cloud base mass flux +!! is further reduced in proportion to the ratio of tauadv to dtconv. if(asqecflg(i)) then tfac = tauadv(i) / dtconv(i) tfac = min(tfac, 1.) @@ -2018,6 +2345,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo !! +!> - If the large scale destabilization is less than zero, or the +!! stabilization by the convection is greater than zero, then the scheme +!! returns to the calling routine without modifying the state variables. totflg = .true. do i=1,im totflg = totflg .and. (.not. cnvflg(i)) @@ -2025,9 +2355,11 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & if(totflg) return !! ! -!--- modified Grell & Freitas' (2014) updraft fraction which uses -! actual entrainment rate at cloud base -! +!> - For scale-aware parameterization, the updraft fraction (sigmagfm) +!! is first computed as a function of the lateral entrainment rate at +!! cloud base (see Han et al.'s (2017) \cite han_et_al_2017 equation +!! 4 and 5), following the study by Grell and Freitas (2014) +!! \cite grell_and_freitas_2014. do i = 1, im if(cnvflg(i)) then tem = min(max(xlamx(i), 7.e-5), 3.e-4) @@ -2039,8 +2371,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo ! -!--- compute scale-aware function based on Arakawa & Wu (2013) -! +!> - Then, calculate the reduction factor (scaldfunc) of the vertical +!! convective eddy transport of mass flux as a function of updraft +!! fraction from the studies by Arakawa and Wu (2013) +!! \cite arakawa_and_wu_2013 (also see Han et al.'s (2017) +!! \cite han_et_al_2017 equation 1 and 2). The final cloud base mass +!! flux with scale-aware parameterization is obtained from the mass flux +!! when sigmagfm << 1, multiplied by the reduction factor +!! (Han et al.'s (2017) \cite han_et_al_2017 equation 2). do i = 1, im if(cnvflg(i)) then if (gdx(i) < dxcrtuf) then @@ -2076,6 +2414,15 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c--- multiplied by the mass flux necessary to keep the c--- equilibrium with the larger-scale. c +!> ## For the "feedback" control, calculate updated values of the state +!! variables by multiplying the cloud base mass flux and the tendencies +!! calculated per unit cloud base mass flux from the static control. +!> - Calculate the temperature tendency from the moist static energy and +!! specific humidity tendencies. +!> - Update the temperature, specific humidity, and horiztonal wind state +!! variables by multiplying the cloud base mass flux-normalized tendencies +!! by the cloud base mass flux. +!> - Accumulate column-integrated tendencies. do i = 1, im delhbar(i) = 0. delqbar(i) = 0. @@ -2106,6 +2453,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo +!> - Recalculate saturation specific humidity using the updated temperature. do k = 1, km do i = 1, im if (cnvflg(i) .and. k <= kmax(i)) then @@ -2119,6 +2467,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo c +!> - Add up column-integrated convective precipitation by multiplying +!! the normalized value by the cloud base mass flux. do i = 1, im rntot(i) = 0. delqev(i) = 0. @@ -2139,6 +2489,12 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo +!> - Determine the evaporation of the convective precipitation and update +!! the integrated convective precipitation. +!> - Update state temperature and moisture to account for evaporation +!! of convective precipitation. +!> - Update column-integrated tendencies to account for evaporation of +!! convective precipitation. do k = km, 1, -1 do i = 1, im if (k <= kmax(i)) then @@ -2221,6 +2577,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c convective cloud water c +!> - Calculate convective cloud water. do k = 1, km do i = 1, im if (cnvflg(i) .and. rn(i) > 0.) then @@ -2233,6 +2590,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c convective cloud cover c +!> - Calculate convective cloud cover, which is used when pdf-based cloud +!! fraction is used (i.e., pdfcld=.true.). do k = 1, km do i = 1, im if (cnvflg(i) .and. rn(i) > 0.) then @@ -2248,6 +2607,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c cloud water c +!> - Separate detrained cloud water into liquid and ice species as a +!! function of temperature only. if (ncloud > 0) then ! do k = 1, km @@ -2270,6 +2631,8 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! endif c +!> - If convective precipitation is zero or negative, reset the updated +!! state variables back to their original values (negating convective changes). do k = 1, km do i = 1, im if(cnvflg(i) .and. rn(i) <= 0.) then @@ -2285,6 +2648,9 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! ! hchuang code change ! +!> - Calculate and retain the updraft and downdraft mass fluxes for dust transport by cumulus convection. +! +!> - Calculate the updraft convective mass flux. do k = 1, km do i = 1, im if(cnvflg(i) .and. rn(i) > 0.) then @@ -2294,12 +2660,14 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo +!> - save the updraft convective mass flux at cloud top. do i = 1, im if(cnvflg(i) .and. rn(i) > 0.) then k = ktop(i)-1 dt_mf(i,k) = ud_mf(i,k) endif enddo +!> - Calculate the downdraft convective mass flux. do k = 1, km do i = 1, im if(cnvflg(i) .and. rn(i) > 0.) then @@ -2312,7 +2680,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & !! return end subroutine sasasdeep_run - !> @} - !> @} +!! @} +!! @} end module sasas_deep diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 9bc8b1f83..174b9bcbb 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -1,14 +1,38 @@ !> \file mfshalcnv.f -!! This file contains the Scale-Aware mass flux Shallow Convection scheme. - - module sasas_shal - contains - -!> \defgroup SASHAL Scale-Aware Mass Flux Shallow Convection +!! This file contains the entire SAMF deep convection scheme. +!> \defgroup SAMF_shal Scale-Aware Mass-Flux Shallow Convection !! @{ -!! \brief Brief description of the parameterization +!! \brief The scale-aware mass-flux shallow (SAMF_shal) convection +!! scheme is an updated version of the previous mass-flux shallow +!! convection scheme with scale and aerosol awareness and +!! parameterizes the effect of shallow convection on the environment. +!! The SAMF_shal scheme is similar to the SAMF deep convection scheme +!! but with a few key differences. First, no quasi-equilibrium assumption +!! is used for any grid size and the shallow cloud base mass flux is +!! parameterized using a mean updraft velocity. Further, there are no +!! convective downdrafts, the entrainment rate is greater than for deep +!! convection, and the shallow convection is limited to not extend over +!! the level where \f$p=0.7p_{sfc}\f$. The paramerization of scale and +!! aerosol awareness follows that of the SAMF deep convection scheme. +!! +!! The previous version of the shallow convection scheme (shalcnv.f) +!! is described in Han and Pan (2011) \cite han_and_pan_2011 and differences +!! between the shallow and deep convection schemes are presented in +!! Han and Pan (2011) \cite han_and_pan_2011 and Han et al. (2017) +!! \cite han_et_al_2017 . Details of scale- and aerosol-aware parameterizations +!! are described in Han et al. (2017) \cite han_et_al_2017 . +!! !! \section diagram Calling Hierarchy Diagram +!! \image html SAMF_shal_Flowchart.png "Diagram depicting how the SAMF +!! shallow convection scheme is called from the FV3GFS physics time loop" +!! height=2cm !! \section intraphysics Intraphysics Communication +!! This space is reserved for a description of how this scheme uses +!! information from other scheme types and/or how information calculated +!! in this scheme is used in other scheme types. + + module sasas_shal + contains !> \brief Brief description of the subroutine !! @@ -17,7 +41,14 @@ module sasas_shal subroutine sasasshal_init end subroutine sasasshal_init -!> \brief Brief description of the subroutine +!> \brief The subroutine contains the entirety of the SAMF shallow convection scheme. +!! This routine follows the \ref SAMF deep scheme quite closely, although +!! it can be interpreted as only having the "static" and "feedback" control +!! portions, since the "dynamic" control is not necessary to find the +!! cloud base mass flux. The algorithm is simplified from SAMF deep +!! convection by excluding convective downdrafts and being confined to +!! operate below \f$p=0.7p_{sfc}\f$. Also, entrainment is both simpler +!! and stronger in magnitude compared to the deep scheme. !! !! \section arg_table_sasasshal_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -51,6 +82,17 @@ end subroutine sasasshal_init !! | cnvc | convective_cloud_cover | convective cloud cover | frac | 2 | real | kind_phys | out | F | !! !! \section general General Algorithm +!! -# Compute preliminary quantities needed for the static and feedback +!! control portions of the algorithm. +!! -# Perform calculations related to the updraft of the entraining/detraining +!! cloud model ("static control"). +!! -# The cloud base mass flux is obtained using the cumulus updraft +!! velocity averaged ove the whole cloud depth. +!! -# Calculate the tendencies of the state variables (per unit cloud +!! base mass flux) and the cloud base mass flux. +!! -# For the "feedback control", calculate updated values of the state +!! variables by multiplying the cloud base mass flux and the tendencies +!! calculated per unit cloud base mass flux from the static control. !! \section detailed Detailed Algorithm !! @{ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & @@ -1494,7 +1536,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & !! return end subroutine sasasshal_run -!> @} +!! @} !> \brief Brief description of the subroutine !! @@ -1502,7 +1544,7 @@ end subroutine sasasshal_run !! subroutine sasasshal_finalize end subroutine sasasshal_finalize -!> @} +!! @} end module sasas_shal diff --git a/physics/radlw_main.f b/physics/radlw_main.f index f132a1e81..456a9fdab 100644 --- a/physics/radlw_main.f +++ b/physics/radlw_main.f @@ -2,6 +2,95 @@ !! This file contains NCEP's modifications of the rrtmg-lw radiation !! code from AER. +!>\defgroup RRTMG GFS RRTMG Shortwave/Longwave Radiation Scheme +!! @{ +!! \brief The GFS radiation scheme +!! \details Radiative processes are among the most complex and +!! computationally intensive parts of all model physics. As an +!! essential component of modeling the atmosphere, radiation directly +!! and indirectly connects all physics processes with model dynamics, +!! and it regulates the overall earth-atmosphere energy exchanges and +!! transformations. +!! +!! The schematic radiation module structure is shown in Table 1. +!! \image html schematic_Rad_mod.png "Table 1: Schematic Radiation Module Structure" width=10cm +!! +!> GFS radiation package is intended to provide a fast and accurate +!! method of determining the total radiative flux at any given +!! location. These calculations provide both the total radiative flux +!! at the ground surface, which is needed to establish the surface +!! energy budget, and the vertical radiative flux divergence, which is +!! used to calculate the radiative heating and cooling rates of a given +!! atmospheric layer. The magnitude of the terms in the surface energy +!! budget can set the stage for moist deep convection and are crucial +!! to the formation of low-level clouds. In addition, the vertical +!! radiative flux divergence can produce substantial cooling, +!! particularly at the tops of clouds, which can have strong dynamical +!! effects on cloud evolution. +!! +!! It uses a correlated-k distribution method and a transmittance lookup +!! table that is linearly scaled by optical depth to achieve high +!! accuracy and efficiency. The algorithm contains 140 unevenly +!! distributed quadrature points (reduced from the original set of 256) +!! to integrate the cumulative probability distribution functions of +!! absorption over 16 spectral bands. It employs the +!! Clough-Kneizys-Davies (CKD_2.4) continuum model (Clough et al. 1992 +!! \cite clough_et_al_1992) to compute absorption by water vapor at the +!! continuum band. Longwave cloud radiative properties external to the +!! RRTM depend on cloud liquid/ice water path and the effective radius +!! of ice particles and water droplets (Hu and Stamnes 1993 \cite +!! hu_and_stamnes_1993; Ebert and Curry 1992 \cite ebert_and_curry_1992). +!! +!! Changes to Radiation Parameterization since 2007: +!! \n The longwave (LW) and the shortwave (SW) radiation +!! parameterizations in NCEP's operational GFS are both modified and +!! optimized versions of the Rapid Radiative Transfer Model for GCMs +!! (RRTMG_LW v2.3 and RRTMG_SW v2.3, respectively) developed at AER +!! (Iacono et al. 2008 \cite iacono_et_al_2008,Mlawer et al. 1997 +!! \cite mlawer_et_al_1997, Iacono et al., 2000 \cite iacono_et_al_2000, +!! Clough et al., 2005 \cite clough_et_al_2005). The LW algorithm +!! contains 140 unevenly distributed g-points (quadrature points) in 16 +!! broad spectral bands, while the SW algorithm includes 112 g-points +!! in 14 bands. In addition to the major atmospheric absorbing gases of +!! ozone, water vapor, and carbon dioxide, the algorithm also includes +!! various minor absorbing species such as methane, nitrous oxide, +!! oxygen, and in the longwave up to four types of halocarbons (CFCs). +!! To represent statistically the unresolved subgrid cloud variability +!! when dealing multi layered clouds, a Monte-Carlo Independent Column +!! Approximation (McICA) method is used in the RRTMG radiative transfer. +!! A maximum-random cloud overlap method is used in both LW and SW +!! radiation calculations. Cloud condensate path and effective radius +!! for water and ice are used for the calculation of cloud-radiative +!! properties. Hu and Stamnes's method (1993) \cite hu_and_stamnes_1993 +!! is used to treat water clouds in both LW and SW parameterizations. +!! For ice clouds. Fu's parameterizations (1996,1998) \cite fu_1996 +!! \cite fu_et_al_1998 are used in the SW and LW, respectively. +!! +!! In the operational GFS, a climatological tropospheric aerosol with +!! a 5-degree horizontal resolution is used in both LW and SW +!! radiations. A generalized spectral mapping formulation was developed +!! to compute radiative properties of various aerosol components for +!! each of the radiation spectral bands. A separate stratospheric +!! volcanic aerosol parameterization was added that is capable of +!! handling volcanic events. In SW, a new table of incoming solar +!! constants is derived covering time period of 1850-2019 (Vandendool, +!! personal communivation). An eleven-year solar cycle approximation +!! will be used for time out of the window period in long term climate +!! simulations. The SW albedo parameterization uses surface vegetation +!! type based seasonal climatology similar to that described in the +!! NCEP OFFICE Note 441 (Hou et al. 2002 \cite hou_et_al_2002) but with +!! a modification in the treatment of solar zenith angle dependency over +!! snow-free land surface (Yang et al. 2008 \cite yang_et_al_2008). +!! Similarly, vegetation type based non-black-body surface emissivity +!! is used for the LW radiation. Concentrations of atmospheric +!! greenhouse gases are either obtained from global network +!! measurements, such as carbon dioxide (CO2), or taking the +!! climatological constants, the actual CO2 value for the forecast time +!! is an estimation based on the most recent five-year observations. In +!! the lower atmosphere (<3km) a monthly mean CO2 distribution in 15 +!! degree horizontal resolution is used, while a global mean monthly +!! value is used in the upper atmosphere. +! !!!!! ============================================================== !!!!! !!!!! lw-rrtm3 radiation package description !!!!! !!!!! ============================================================== !!!!! @@ -6726,3 +6815,4 @@ end module module_radlw_main ! !========================================! !! @} +!! @} diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index 075bf3dac..24b50fb50 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -364,7 +364,7 @@ subroutine sfc_ex_coef_run & return end subroutine sfc_ex_coef_run -!> @} +!! @} end module surface_exchange_coefficients -!> @} +!! @} diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index c205a96ea..179cb7618 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -1,11 +1,13 @@ !> \file sfc_drv.f !! This file contains the NOAH land surface scheme. -!> \defgroup NOAH NOAH Land Surface pre +!> \defgroup NOAH NOAH Land Surface Scheme +!! \brief This is the NOAH land surface scheme. +!! @{ +!> \defgroup NOAH_pre NOAH Land Surface Pre +!! \ingroup NOAH !! @{ !! \brief Brief description of the parameterization -!! \section diagram Calling Hierarchy Diagram -!! \section intraphysics Intraphysics Communication module lsm_noah_pre contains @@ -63,12 +65,13 @@ subroutine lsm_noah_pre_run & end subroutine lsm_noah_pre_run -!> @} +!! @} end module lsm_noah_pre -!> @} +!! @} -!> \defgroup NOAH NOAH Land Surface post +!> \defgroup NOAH_post NOAH Land Surface post +!! \ingroup NOAH !! @{ !! \brief Brief description of the parameterization !! \section diagram Calling Hierarchy Diagram @@ -125,11 +128,12 @@ subroutine lsm_noah_post_run & end subroutine lsm_noah_post_run -!> @} +!! @} end module lsm_noah_post -!> @} +!! @} -!> \defgroup NOAH NOAH Land Surface +!> \defgroup NOAH_main NOAH Land Surface Main +!! \ingroup NOAH !! @{ !! \brief Brief description of the parameterization !! \section diagram Calling Hierarchy Diagram @@ -764,7 +768,8 @@ subroutine lsm_noah_run & ! end subroutine sfc_drv end subroutine lsm_noah_run !----------------------------------- -!> @} +!! @} end module lsm_noah -!> @} +!! @} +!! @} From 47ba78a2bf2a88bbc10d1e61aa0f29a58e12b604 Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Mon, 22 Jan 2018 21:21:10 -0700 Subject: [PATCH 03/22] currently documenting main subroutine of each physics scheme --- physics/GFS_RRTMG_pre.f90 | 102 --------------------------- physics/GFS_calpreciptype.f90 | 10 +-- physics/docs/ccpp_dox | 2 +- physics/gscond.f | 24 +++---- physics/gwdc.f | 97 +++++++------------------- physics/gwdps.f | 125 +++++++++++----------------------- physics/mfdeepcnv.f | 44 ++++++------ physics/mfpbl.f | 2 +- physics/mfshalcnv.f | 35 +++++----- physics/moninedmf.f | 3 +- physics/ozphys.f | 59 ++++++---------- physics/precpd.f | 20 +++--- physics/radlw_main.f | 63 +---------------- physics/radsw_main.f | 70 +------------------ physics/sfc_diff.f | 6 +- physics/sfc_drv.f | 36 +++++----- physics/sfc_nst.f | 18 ++--- physics/sfc_sice.f | 30 ++++---- 18 files changed, 200 insertions(+), 546 deletions(-) diff --git a/physics/GFS_RRTMG_pre.f90 b/physics/GFS_RRTMG_pre.f90 index a44d3e262..2a490bf42 100644 --- a/physics/GFS_RRTMG_pre.f90 +++ b/physics/GFS_RRTMG_pre.f90 @@ -1,106 +1,5 @@ !> \file GFS_RRTMG_pre.f90 !! This file contains -!> \defgroup RRTMG GFS RRTMG Shortwave/Longwave Radiation Scheme -!! @{ -!! \brief The GFS radiation scheme -!! \details Radiative processes are among the most complex and -!! computationally intensive parts of all model physics. As an -!! essential component of modeling the atmosphere, radiation directly -!! and indirectly connects all physics processes with model dynamics, -!! and it regulates the overall earth-atmosphere energy exchanges and -!! transformations. -!! -!! The radiation package in GFS physics has standardized component -!! modules (Table 1). The radiation driver module (\ref -!! module_radiation_driver) is the interface with the Interoperable -!! Physics Driver (IPD) for NGGPS, and it has three subroutines called -!! by IPD (Figure 1): -!! - radinit() is called in subroutine nuopc_phys_init to set up -!! radiation related fixed parameters. -!! - radupdate() is called in subroutine nuopc_rad_update to update -!! values between timesteps. -!! - grrad() is called in subroutine nuopc_rad_run, and it is the -!! driver of radiation calculation. -!! \image html ipd_rad.png "Figure 1: Schematic illustration of the communication between the GFS radiation package and IPD " width=10cm -!! -!! The schematic radiation module structure is shown in Table 1. -!! \image html schematic_Rad_mod.png "Table 1: Schematic Radiation Module Structure" width=10cm -!! -!> GFS radiation package is intended to provide a fast and accurate -!! method of determining the total radiative flux at any given -!! location. These calculations provide both the total radiative flux -!! at the ground surface, which is needed to establish the surface -!! energy budget, and the vertical radiative flux divergence, which is -!! used to calculate the radiative heating and cooling rates of a given -!! atmospheric layer. The magnitude of the terms in the surface energy -!! budget can set the stage for moist deep convection and are crucial -!! to the formation of low-level clouds. In addition, the vertical -!! radiative flux divergence can produce substantial cooling, -!! particularly at the tops of clouds, which can have strong dynamical -!! effects on cloud evolution. -!! -!! It uses a correlated-k distribution method and a transmittance lookup -!! table that is linearly scaled by optical depth to achieve high -!! accuracy and efficiency. The algorithm contains 140 unevenly -!! distributed quadrature points (reduced from the original set of 256) -!! to integrate the cumulative probability distribution functions of -!! absorption over 16 spectral bands. It employs the -!! Clough-Kneizys-Davies (CKD_2.4) continuum model (Clough et al. 1992 -!! \cite clough_et_al_1992) to compute absorption by water vapor at the -!! continuum band. Longwave cloud radiative properties external to the -!! RRTM depend on cloud liquid/ice water path and the effective radius -!! of ice particles and water droplets (Hu and Stamnes 1993 \cite -!! hu_and_stamnes_1993; Ebert and Curry 1992 \cite ebert_and_curry_1992). -!! -!! Changes to Radiation Parameterization since 2007: -!! \n The longwave (LW) and the shortwave (SW) radiation -!! parameterizations in NCEP's operational GFS are both modified and -!! optimized versions of the Rapid Radiative Transfer Model for GCMs -!! (RRTMG_LW v2.3 and RRTMG_SW v2.3, respectively) developed at AER -!! (Iacono et al. 2008 \cite iacono_et_al_2008,Mlawer et al. 1997 -!! \cite mlawer_et_al_1997, Iacono et al., 2000 \cite iacono_et_al_2000, -!! Clough et al., 2005 \cite clough_et_al_2005). The LW algorithm -!! contains 140 unevenly distributed g-points (quadrature points) in 16 -!! broad spectral bands, while the SW algorithm includes 112 g-points -!! in 14 bands. In addition to the major atmospheric absorbing gases of -!! ozone, water vapor, and carbon dioxide, the algorithm also includes -!! various minor absorbing species such as methane, nitrous oxide, -!! oxygen, and in the longwave up to four types of halocarbons (CFCs). -!! To represent statistically the unresolved subgrid cloud variability -!! when dealing multi layered clouds, a Monte-Carlo Independent Column -!! Approximation (McICA) method is used in the RRTMG radiative transfer. -!! A maximum-random cloud overlap method is used in both LW and SW -!! radiation calculations. Cloud condensate path and effective radius -!! for water and ice are used for the calculation of cloud-radiative -!! properties. Hu and Stamnes's method (1993) \cite hu_and_stamnes_1993 -!! is used to treat water clouds in both LW and SW parameterizations. -!! For ice clouds. Fu's parameterizations (1996,1998) \cite fu_1996 -!! \cite fu_et_al_1998 are used in the SW and LW, respectively. -!! -!! In the operational GFS, a climatological tropospheric aerosol with -!! a 5-degree horizontal resolution is used in both LW and SW -!! radiations. A generalized spectral mapping formulation was developed -!! to compute radiative properties of various aerosol components for -!! each of the radiation spectral bands. A separate stratospheric -!! volcanic aerosol parameterization was added that is capable of -!! handling volcanic events. In SW, a new table of incoming solar -!! constants is derived covering time period of 1850-2019 (Vandendool, -!! personal communivation). An eleven-year solar cycle approximation -!! will be used for time out of the window period in long term climate -!! simulations. The SW albedo parameterization uses surface vegetation -!! type based seasonal climatology similar to that described in the -!! NCEP OFFICE Note 441 (Hou et al. 2002 \cite hou_et_al_2002) but with -!! a modification in the treatment of solar zenith angle dependency over -!! snow-free land surface (Yang et al. 2008 \cite yang_et_al_2008). -!! Similarly, vegetation type based non-black-body surface emissivity -!! is used for the LW radiation. Concentrations of atmospheric -!! greenhouse gases are either obtained from global network -!! measurements, such as carbon dioxide (CO2), or taking the -!! climatological constants, the actual CO2 value for the forecast time -!! is an estimation based on the most recent five-year observations. In -!! the lower atmosphere (<3km) a monthly mean CO2 distribution in 15 -!! degree horizontal resolution is used, while a global mean monthly -!! value is used in the upper atmosphere. module GFS_RRTMG_pre @@ -716,6 +615,5 @@ end subroutine GFS_RRTMG_pre_finalize !! @} end module GFS_RRTMG_pre -!! @} diff --git a/physics/GFS_calpreciptype.f90 b/physics/GFS_calpreciptype.f90 index 17ecf30c7..587af6d77 100644 --- a/physics/GFS_calpreciptype.f90 +++ b/physics/GFS_calpreciptype.f90 @@ -7,12 +7,12 @@ module GFS_calpreciptype contains - -!> \section arg_table_GFS_calpreciptype_init Argument Table -!! +! \section arg_table_GFS_calpreciptype_init Argument Table +! subroutine GFS_calpreciptype_init end subroutine GFS_calpreciptype_init +!>\defgroup gfs_calpreciptype GFS calpreciptype Main !> \section arg_table_GFS_calpreciptype_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------|------------------------------------------------------------|---------|------|---------|-----------|--------|----------| @@ -1516,8 +1516,8 @@ subroutine calwxt_dominant(nalg,rain,freezr,sleet,snow, & return end subroutine calwxt_dominant -!> \section arg_table_GFS_calpreciptype_finalize Argument table -!! +! \section arg_table_GFS_calpreciptype_finalize Argument table +! subroutine GFS_calpreciptype_finalize end subroutine GFS_calpreciptype_finalize diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index 53cdc1445..2aa09a7b3 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -1,6 +1,6 @@ # Doxyfile 1.8.11 DOXYFILE_ENCODING = UTF-8 -PROJECT_NAME = "CCPP Physics Documentation" +PROJECT_NAME = "GMTB CCPP Physics Documentation" PROJECT_NUMBER = "" PROJECT_BRIEF = "" PROJECT_LOGO = img/dtc_logo.png diff --git a/physics/gscond.f b/physics/gscond.f index 636666174..31f2040b0 100644 --- a/physics/gscond.f +++ b/physics/gscond.f @@ -6,7 +6,7 @@ module GFS_zhaocarr_gscond contains -!> \defgroup Zhao-Carr Zhao-Carr Microphysics +!> \defgroup Zhao-Carr GFS Zhao-Carr Microphysics !! @{ !! \brief The GFS scheme for large-scale condensation and precipitation !! , based on Zhao and Carr (1997) \cite zhao_and_carr_1997 @@ -37,22 +37,19 @@ module GFS_zhaocarr_gscond !! - EVPCO: Coefficient for evaporation of precipitation !! !! \section intramps Intraphysics Communication -!! - Routine GSCOND is called from GBPHYS after call to SHALCNV -!! - Routine PRECPD is called from GBPHYS after call to GSCOND !> \defgroup condense Grid-Scale Condensation and Evaporation of Cloud !! @{ -!> \ingroup condense -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gscond_init Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_gscond_init Argument Table +! subroutine gscond_init end subroutine gscond_init -!> \ingroup condense +!> \defgroup gfs_gscond GFS gscond Main !! \brief This subroutine computes grid-scale condensation and evaporation of !! cloud condensate. !! @@ -540,11 +537,10 @@ subroutine gscond_run (im,ix,km,dt,dtf,prsl,ps,q,clw1,clw2 & end subroutine gscond_run !> @} -!> \ingroup condense -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gscond_finalize Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_gscond_finalize Argument Table +! subroutine gscond_finalize end subroutine gscond_finalize diff --git a/physics/gwdc.f b/physics/gwdc.f index 5c86480d3..c48f335ba 100644 --- a/physics/gwdc.f +++ b/physics/gwdc.f @@ -70,18 +70,16 @@ module gwdc_pre contains -!> \ingroup GFS_cgwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdc_pre_init Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_gwdc_pre_init Argument Table !! subroutine gwdc_pre_init () end subroutine gwdc_pre_init -!> \ingroup GFS_cgwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdc_pre_run Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_gwdc_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|--------------------------------------------------------------------------|---------------------------------------------------------------|-------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -149,10 +147,9 @@ subroutine gwdc_pre_run ( & end subroutine gwdc_pre_run -!> \ingroup GFS_cgwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdc_pre_finalize Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_gwdc_pre_finalize Argument Table !! subroutine gwdc_pre_finalize () end subroutine gwdc_pre_finalize @@ -165,16 +162,15 @@ module gwdc contains -!> \ingroup GFS_cgwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdc_init Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_gwdc_init Argument Table !! subroutine gwdc_init() end subroutine gwdc_init -!> \ingroup GFS_cgwd -!! This subroutine is the parameterization of convective gravity wave +!> \defgroup GFS_gwdc_run GFS gwdc Main +!! \brief This subroutine is the parameterization of convective gravity wave !! drag based on the theory given by Chun and Baik (1998) !! \cite chun_and_baik_1998 modified for implementation into the !! GFS/CFS by Ake Johansson(Aug 2005). @@ -199,43 +195,6 @@ end subroutine gwdc_init !! hypothesis in order to find wave breaking levels in terms of the !! Richardon number criterion using the nonlinearity factor of !! thermally induced waves. -!> \param[in] IM horizontal number of used pts -!> \param[in] IX horizontal dimension -!> \param[in] IY horizontal number of used pts -!> \param[in] KM vertical layer dimension -!> \param[in] LAT latitude index - used for debug prints -!> \param[in] U1 u component of layer wind -!> \param[in] V1 v component of layer wind -!> \param[in] T1 layer mean temperature (K) -!> \param[in] Q1 layer mean tracer concentration -!> \param[in] DELTIM physics time step in sectons -!> \param[in] PMID1 mean layer pressure -!> \param[in] PINT1 pressure at layer interfaces -!> \param[in] DPMID1 mean layer delta p -!> \param[in] QMAX maximum convective heating rate (k/s) in a -!! horizontal grid point calculated -!! from cumulus parameterization -!> \param[in] KTOP vertical level index for cloud top -!> \param[in] KBOT vertical level index for cloud bottom -!> \param[in] KCNV (0,1) dependent on whether convection occur or not -!> \param[in] CLDF deep convective cloud fraction at the cloud top -!> \param[in] GRAV gravity defined in physcon -!> \param[in] CP specific heat at constant pressure defined in -!! physcon -!> \param[in] RD gas constant air defined in physcon -!> \param[in] FV con_fvirt = con_rv/con_rd-1 -!> \param[in] PI ratio of a circle's circumference to its diameter -!> \param[in] DLENGTH grid spacing in the direction of basic wind at -!! the cloud top -!> \param[in] LPRNT logical print flag -!> \param[in] IPR check print point for debugging -!> \param[in] FHOUR forecast hour -!> \param[out] UTGWC zonal wind tendency -!> \param[out] VTGWC meridional wind tendency -!> \param[out] TAUCTX wave stress at the cloud top projected in the -!! east -!> \param[out] TAUCTY wave stress at the cloud top projected in the -!! north !! !! \section arg_table_gwdc_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -1557,10 +1516,9 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & end subroutine gwdc_run !> @} -!> \ingroup GFS_cgwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdc_finalize Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_gwdc_finalize Argument Table !! subroutine gwdc_finalize() end subroutine gwdc_finalize @@ -1573,18 +1531,16 @@ module gwdc_post contains -!> \ingroup GFS_cgwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdc_post_init Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_gwdc_post_init Argument Table !! subroutine gwdc_post_init() end subroutine gwdc_post_init -!> \ingroup GFS_cgwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdc_post_run Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_gwdc_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------------|--------------------------------------------------------------------------|------------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | default | in | F | @@ -1656,10 +1612,9 @@ subroutine gwdc_post_run( & end subroutine gwdc_post_run -!> \ingroup GFS_cgwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdc_post_finalize Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_gwdc_post_finalize Argument Table !! subroutine gwdc_post_finalize() end subroutine gwdc_post_finalize diff --git a/physics/gwdps.f b/physics/gwdps.f index a86c2f806..22d78c636 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -96,25 +96,23 @@ !! gravity wave drag than the T383L64 version. !! !!\section intra_gwdps Intraphysics Communication -!! - Routine GWDPS is called from GBPHYS after call -!! to MONINEDMF module gwdps_pre contains -!> \ingroup GFS_ogwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdps_pre_init Argument Table -!! +! \ingroup GFS_ogwd +! \brief Brief description of the subroutine +! +! \section arg_table_gwdps_pre_init Argument Table +! subroutine gwdps_pre_init() end subroutine gwdps_pre_init -!> \ingroup GFS_ogwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdps_pre_run Argument Table +! \ingroup GFS_ogwd +! \brief Brief description of the subroutine +! +! \section arg_table_gwdps_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-------------------------------------------------------------------------|------------------------------------------------------------------------------------------|---------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal dimension | count | 0 | integer | default | in | F | @@ -202,11 +200,11 @@ subroutine gwdps_pre_run( & end subroutine gwdps_pre_run !> @} -!> \ingroup GFS_ogwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdps_pre_finalize Argument Table -!! +! \ingroup GFS_ogwd +! \brief Brief description of the subroutine +! +! \section arg_table_gwdps_pre_finalize Argument Table +! subroutine gwdps_pre_finalize() end subroutine gwdps_pre_finalize @@ -218,15 +216,16 @@ module gwdps contains -!> \ingroup GFS_ogwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdps_init Argument Table -!! +! \ingroup GFS_ogwd +! \brief Brief description of the subroutine +! +! \section arg_table_gwdps_init Argument Table +! subroutine gwdps_init() end subroutine gwdps_init -!> \ingroup GFS_ogwd +!> \defgroup gfs_gwdps GFS gwdps Main +!!\ingroup GFS_ogwd !! \brief This subroutine includes orographic gravity wave drag and mountain !! blocking. !! @@ -279,52 +278,6 @@ end subroutine gwdps_init !! | lprnt | flag_print | flag for debugging printouts | flag | 0 | logical | default | in | F | !! | ipr | horizontal_index_of_printed_column | horizontal index of column used in debugging printouts | index | 0 | integer | default | in | F | !! -!> \param[in] IM horizontal number of used pts -!> \param[in] IX horizontal dimension -!> \param[in] IY horizontal number of used pts -!> \param[in] KM vertical layer dimension -!> \param[in,out] A non-linear tendency for v wind component -!> \param[in,out] B non-linear tendency for u wind component -!> \param[in,out] C non-linear tendency for temperature (not used) -!> \param[in] U1 zonal wind component of model layer wind (m/s) -!> \param[in] V1 meridional wind component of model layer wind -!! (m/s) -!> \param[in] T1 model layer mean temperature (K) -!> \param[in] Q1 model layer mean specific humidity -!> \param[in] KPBL index for the PBL top layer -!> \param[in] PRSI pressure at layer interfaces -!> \param[in] DEL positive increment of p/psfc across layer -!> \param[in] PRSL mean layer pressure -!> \param[in] PRSLK Exner function at layer -!> \param[in] PHII interface geopotential (\f$m^2/s^2\f$) -!> \param[in] PHIL layer geopotential (\f$m^2/s^2\f$) -!> \param[in] DELTIM physics time step in seconds -!> \param[in] KDT number of the current time step -!> \param[in] HPRIME orographic standard deviation (m) (mtnvar(:,1)) -!> \param[in] OC orographic Convexity (mtnvar(:,2)) -!> \param[in] OA4 orographic Asymmetry (mtnvar(:,3:6)) -!> \param[in] CLX4 Lx, the fractional area covered by the -!! subgrid-scale orography higher than a critical height for a grid -!! box with the interval \f$ \triangle x \f$ (mtnvar(:,7:10)) -!> \param[in] THETA the angle of the mtn with that to the east (x) -!! axis (mtnvar(:,11)) -!> \param[in] SIGMA orographic slope (mtnvar(:,13)) -!> \param[in] GAMMA orographic anisotropy (mtnvar(:,12)) -!> \param[in] ELVMAX orographic maximum (mtnvar(:,14)) -!> \param[out] DUSFC u component of surface stress -!> \param[out] DVSFC v component of surface stress -!> \param[in] G see physcons::con_g -!> \param[in] CP see physcons::con_cp -!> \param[in] RD see physcons::con_tird -!> \param[in] RV see physcons::con_rv -!> \param[in] IMX number of longitude points -!> \param[in] NMTVR number of topographic variables such as -!! variance etc used in the GWD parameterization,current operational, -!! nmtvr=14 -!> \param[in] CDMBGWD multiplication factors for cdmb and gwd -!> \param[in] ME pe number - used for debug prints -!> \param[in] LPRNT logical print flag -!> \param[in] IPR check print point for debugging !> \section gen_gwdps General Algorithm !> @{ subroutine gwdps_run( & @@ -1387,11 +1340,11 @@ subroutine gwdps_run( & end subroutine gwdps_run !> @} -!> \ingroup GFS_ogwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdps_finalize Argument Table -!! +! \ingroup GFS_ogwd +! \brief Brief description of the subroutine +! +! \section arg_table_gwdps_finalize Argument Table +! subroutine gwdps_finalize() end subroutine gwdps_finalize @@ -1403,17 +1356,17 @@ module gwdps_post contains -!> \ingroup GFS_ogwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdps_post_init Argument Table -!! +! \ingroup GFS_ogwd +! \brief Brief description of the subroutine +! +! \section arg_table_gwdps_post_init Argument Table +! subroutine gwdps_post_init() end subroutine gwdps_post_init -!> \ingroup GFS_ogwd -!! \brief Brief description of the subroutine -!! \section arg_table_gwdps_post_run Argument Table +! \ingroup GFS_ogwd +! \brief Brief description of the subroutine +! \section arg_table_gwdps_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------|------------------------------------------------------------------|-------|------|---------|-----------|--------|----------| !! | lssav | flag_diagnostics | flag for calculating diagnostic fields | flag | 0 | logical | default | in | F | @@ -1458,11 +1411,11 @@ subroutine gwdps_post_run( & end subroutine gwdps_post_run -!> \ingroup GFS_ogwd -!! \brief Brief description of the subroutine -!! -!! \section arg_table_gwdps_post_finalize Argument Table -!! +! \ingroup GFS_ogwd +! \brief Brief description of the subroutine +! +! \section arg_table_gwdps_post_finalize Argument Table +! subroutine gwdps_post_finalize() end subroutine gwdps_post_finalize diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index bf293e24d..ef6067f46 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -1,6 +1,6 @@ !> \file mfdeepcnv.f !! This file contains the entire SAMF deep convection scheme. -!> \defgroup SAMF Scale-Aware Mass-Flux Deep Convection +!> \defgroup SAMF GFS Scale-Aware Mass-Flux Deep Convection !! @{ !> \brief The scale-aware mass-flux (SAMF) deep convection scheme is an !! updated version of the previous Simplified Arakawa-Schubert (SAS) scheme @@ -69,8 +69,8 @@ module sasas_deep !! \section diagram Calling Hierarchy Diagram !! \section intraphysics Intraphysics Communication -!> \brief Brief description of the subroutine -!! +! \brief Brief description of the subroutine +! ! \section arg_table_sasasdeep_init Argument Table ! | local var name | longname | description | units | rank | type | kind | intent | optional | ! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| @@ -79,8 +79,8 @@ subroutine sasasdeep_init end subroutine sasasdeep_init -!> \brief Brief description of the subroutine -!! +! \brief Brief description of the subroutine +! ! \section arg_table_sasasdeep_finalize Argument Table ! | local var name | longname | description | units | rank | type | kind | intent | optional | ! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| @@ -89,6 +89,7 @@ subroutine sasasdeep_finalize end subroutine sasasdeep_finalize +!>\defgroup GFS_mfdeep GFS mfdeepcnv Main !>\brief This subroutine contains the entirety of the SAMF deep convection scheme. !! !! For grid sizes larger than threshold value, as in Grell (1993) @@ -153,21 +154,20 @@ end subroutine sasasdeep_finalize !! cloud model ("static control"). !! -# Perform calculations related to the downdraft of the entraining/detraining !! cloud model ("static control"). -!! !! -# For grid sizes larger than the threshold value (currently 8 km): -!! - 1) Using the updated temperature and moisture profiles that were +!!\n 1) Using the updated temperature and moisture profiles that were !! modified by the convection on a short time-scale, recalculate the !! total cloud work function to determine the change in the cloud work !! function due to convection, or the stabilizing effect of the cumulus. -!! - 2) For the "dynamic control", using a reference cloud work function, +!!!\n 2) For the "dynamic control", using a reference cloud work function, !! estimate the change in cloud work function due to the large-scale dynamics. !! Following the quasi-equilibrium assumption, calculate the cloud base !! mass flux required to keep the large-scale convective destabilization !! in balance with the stabilization effect of the convection. !! !! -# For grid sizes smaller than the threshold value (currently 8 km): -!! - 1) compute the cloud base mass flux using the cumulus updraft -!! velocity averaged ove the whole cloud depth. +!!\n 1) compute the cloud base mass flux using the cumulus updraft +!! velocity averaged over the whole cloud depth. !! !! -# For scale awareness, the updraft fraction (sigma) is obtained as !! a function of cloud base entrainment. Then, the final cloud base mass @@ -275,7 +275,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & & cinacr, cinacrmx, cinacrmn cj -!> parameters for updraft velocity calculation +! parameters for updraft velocity calculation real(kind=kind_phys) bet1, cd1, f1, gam1, & bb1, bb2, wucb @@ -344,7 +344,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & !> ## Compute preliminary quantities needed for static, dynamic, and feedback control portions of the algorithm. !> - Convert input pressure terms to centibar units. !************************************************************************ -!> convert input Pa terms to Cb terms -- Moorthi +! convert input Pa terms to Cb terms -- Moorthi ps = psp * 0.001 prsl = prslp * 0.001 del = delp * 0.001 @@ -499,13 +499,15 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c hydrostatic height assume zero terr and initially assume c updraft entrainment rate as an inverse function of height c -!> - Calculate hydrostatic height at layer centers assuming a flat surface (no terrain) from the geopotential. +!> - Calculate hydrostatic height at layer centers assuming a flat +!! surface (no terrain) from the geopotential. do k = 1, km do i=1,im zo(i,k) = phil(i,k) / g enddo enddo -!> - Calculate interface height and the initial entrainment rate as an inverse function of height. +!> - Calculate interface height and the initial entrainment rate as +!! an inverse function of height. do k = 1, km1 do i=1,im zi(i,k) = 0.5*(zo(i,k)+zo(i,k+1)) @@ -517,7 +519,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! c convert surface pressure to mb from cb c -!> - Convert prsl from centibar to millibar, set normalized mass fluxes +!> - Convert \a prsl from centibar to millibar, set normalized mass fluxes !! to 1, cloud properties to 0, and save model state variables (after !! advection/turbulence). do k = 1, km @@ -1492,8 +1494,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c - compute precipitation efficiency in terms of windshear c -!> ## Perform calculations related to the downdraft of the entraining/detraining -!! cloud model ("static control"). +!> ## Perform calculations related to the downdraft of the entraining/detraining cloud model ("static control"). !! - First, in order to calculate the downdraft mass flux (as a fraction !! of the updraft mass flux), calculate the wind shear and precipitation !! efficiency according to equation 58 in Fritsch and Chappell (1980) @@ -1900,10 +1901,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c--- environmental conditions again, first heights c -!> ## Using the updated temperature and moisture profiles that were -!! modified by the convection on a short time-scale, recalculate the -!! total cloud work function to determine the change in the cloud work -!! function due to convection, or the stabilizing effect of the cumulus. +!> ## Using the updated temperature and moisture profiles that were modified by the convection on a short time-scale, recalculate the total cloud work function to determine the change in the cloud work function due to convection, or the stabilizing effect of the cumulus. !! - Using notation from Pan and Wu (1995) \cite pan_and_wu_1995, the !! previously calculated cloud work function is denoted by \f$A^+\f$. !! Now, it is necessary to use the entraining/detraining cloud model @@ -2414,9 +2412,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & c--- multiplied by the mass flux necessary to keep the c--- equilibrium with the larger-scale. c -!> ## For the "feedback" control, calculate updated values of the state -!! variables by multiplying the cloud base mass flux and the tendencies -!! calculated per unit cloud base mass flux from the static control. +!> ## For the "feedback" control, calculate updated values of the state variables by multiplying the cloud base mass flux and the tendencies calculated per unit cloud base mass flux from the static control. !> - Calculate the temperature tendency from the moist static energy and !! specific humidity tendencies. !> - Update the temperature, specific humidity, and horiztonal wind state diff --git a/physics/mfpbl.f b/physics/mfpbl.f index b510f658b..b368078b9 100644 --- a/physics/mfpbl.f +++ b/physics/mfpbl.f @@ -1,7 +1,7 @@ !> \file mfpbl.f !! This file contains the subroutine that calculates the updraft properties and mass flux for use in the Hybrid EDMF PBL scheme. -!> \ingroup HEDMF +!> \ingroup GFS_edmf_main !! \brief This subroutine is used for calculating the mass flux and updraft properties. !! !! The mfpbl routines works as follows: if the PBL is convective, first, the ascending parcel entrainment rate is calculated as a function of height. Next, a surface parcel is initiated according to surface layer properties and the updraft buoyancy is calculated as a function of height. Next, using the buoyancy and entrainment values, the parcel vertical velocity is calculated using a well known steady-state budget equation. With the profile of updraft vertical velocity, the PBL height is recalculated as the height where the updraft vertical velocity returns to 0, and the entrainment profile is updated with the new PBL height. Finally, the mass flux profile is calculated using the updraft vertical velocity and assumed updraft fraction and the updraft properties are calculated using the updated entrainment profile, surface values, and environmental profiles. diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 174b9bcbb..80892c309 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -1,6 +1,6 @@ !> \file mfshalcnv.f !! This file contains the entire SAMF deep convection scheme. -!> \defgroup SAMF_shal Scale-Aware Mass-Flux Shallow Convection +!> \defgroup SAMF_shal GFS Scale-Aware Mass-Flux Shallow Convection !! @{ !! \brief The scale-aware mass-flux shallow (SAMF_shal) convection !! scheme is an updated version of the previous mass-flux shallow @@ -34,13 +34,14 @@ module sasas_shal contains -!> \brief Brief description of the subroutine -!! -!! \section arg_table_sasasshal_init Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_init Argument Table +! subroutine sasasshal_init end subroutine sasasshal_init +!>\defgroup SAMF_shal_main GFS mfshalcnv Main !> \brief The subroutine contains the entirety of the SAMF shallow convection scheme. !! This routine follows the \ref SAMF deep scheme quite closely, although !! it can be interpreted as only having the "static" and "feedback" control @@ -1538,10 +1539,10 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & end subroutine sasasshal_run !! @} -!> \brief Brief description of the subroutine -!! -!! \section arg_table_sasasshal_init Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_init Argument Table +! subroutine sasasshal_finalize end subroutine sasasshal_finalize !! @} @@ -1551,10 +1552,10 @@ end module sasas_shal module sasas_shal_post contains -!> \brief Brief description of the subroutine -!! -!! \section arg_table_sasasshal_post_run Argument Table -!! | local var name | longname | description | units | rank | type | kind | intent | optional | +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_post_run Argument Table +! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|----------------------------------------------------------|----------------------------------------------------------------------|---------|------|-------------------------------|-----------|--------|----------| !! | frain | dynamics_to_physics_timestep_ratio | ratio of dynamics timestep to physics timestep | none | 0 | real | kind_phys | in | F | !! | rain1 | lwe_thickness_of_shallow_convective_precipitation_amount | shallow convective rainfall amount on physics timestep | m | 1 | real | kind_phys | in | F | @@ -1611,10 +1612,10 @@ end subroutine sasasshal_post_run subroutine sasasshal_post_init () end subroutine sasasshal_post_init -!> \brief Brief description of the subroutine -!! -!! \section arg_table_sasasshal_post_finalize Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_post_finalize Argument Table +! subroutine sasasshal_post_finalize () end subroutine sasasshal_post_finalize diff --git a/physics/moninedmf.f b/physics/moninedmf.f index 2f3dd715d..bb6d3f6c9 100644 --- a/physics/moninedmf.f +++ b/physics/moninedmf.f @@ -6,7 +6,7 @@ module edmf contains -!> \defgroup HEDMF Hybrid Eddy-diffusivity Mass-flux PBL and Free Atmospheric Turbulence +!> \defgroup HEDMF GFS Hybrid Eddy-diffusivity Mass-flux PBL and Free Atmospheric Turbulence !! @{ !! \brief The Hybrid EDMF scheme is a first-order turbulent transport scheme used for subgrid-scale vertical turbulent mixing in the PBL and above. It blends the traditional first-order approach that has been used and improved over the last several years with a more recent scheme that uses a mass-flux approach to calculate the countergradient diffusion terms. !! @@ -23,6 +23,7 @@ end subroutine edmf_init subroutine edmf_finalize () end subroutine edmf_finalize +!>\defgroup GFS_edmf_main GFS moninedmf Main !> \brief This subroutine contains all of logic for the Hybrid EDMF PBL scheme except for the calculation of the updraft properties and mass flux. !! !! The scheme works on a basic level by calculating background diffusion coefficients and updating them according to which processes are occurring in the column. The most important difference in diffusion coefficients occurs between those levels in the PBL and those above the PBL, so the PBL height calculation is of utmost importance. An initial estimate is calculated in a "predictor" step in order to calculate Monin-Obukhov similarity values and a corrector step recalculates the PBL height based on updated surface thermal characteristics. Using the PBL height and the similarity parameters, the diffusion coefficients are updated below the PBL top based on Hong and Pan (1996) \cite hong_and_pan_1996 (including counter-gradient terms). Diffusion coefficients in the free troposphere (above the PBL top) are calculated according to Louis (1979) \cite louis_1979 with updated Richardson number-dependent functions. If it is diagnosed that PBL top-down mixing is occurring according to Lock et al. (2000) \cite lock_et_al_2000 , then then diffusion coefficients are updated accordingly. Finally, for convective boundary layers (defined as when the Obukhov length exceeds a threshold), the counter-gradient terms are replaced using the mass flux scheme of Siebesma et al. (2007) \cite siebesma_et_al_2007 . In order to return time tendencies, a fully implicit solution is found using tridiagonal matrices, and time tendencies are "backed out." Before returning, the time tendency of temperature is updated to reflect heating due to TKE dissipation following Han et al. (2015) \cite han_et_al_2015 . diff --git a/physics/ozphys.f b/physics/ozphys.f index 3c39ab014..635248c4d 100644 --- a/physics/ozphys.f +++ b/physics/ozphys.f @@ -2,7 +2,7 @@ !! This file is ozone sources and sinks. !> \defgroup GFS_ozn GFS Ozone Sources and Sinks -!! The operational GFS currently parameterizes ozone production and +!! \detail The operational GFS currently parameterizes ozone production and !! destruction based on monthly mean coefficients provided by Naval !! Research Laboratory through CHEM2D chemistry model !! (McCormack et al. 2006 \cite mccormack_et_al_2006). @@ -13,29 +13,27 @@ !! NASA 2D Chemistry model - GSM is capable of running both versions !! !! \section intra_oz Intraphysics Communication -!! - Routine OZPHYS is called from GBPHYS after call to RAYLEIGH_DAMP +!! !! @{ - - module ozphys_pre contains -!! \section arg_table_ozphys_pre_init Argument Table -!! +! \section arg_table_ozphys_pre_init Argument Table +! subroutine ozphys_pre_init() end subroutine ozphys_pre_init -!! \section arg_table_ozphys_pre_run Argument Table -!! +! \section arg_table_ozphys_pre_run Argument Table +! subroutine ozphys_pre_run() end subroutine ozphys_pre_run -!! \section arg_table_ozphys_pre_finalize Argument Table -!! +! \section arg_table_ozphys_pre_finalize Argument Table +! subroutine ozphys_pre_finalize() end subroutine ozphys_pre_finalize @@ -49,15 +47,15 @@ module ozphys contains -!> \ingroup GFS_ozphys -!! \brief Brief description of the subroutine -!! -!! \section arg_table_ozphys_init Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_ozphys_init Argument Table !! subroutine ozphys_init() end subroutine ozphys_init -!> +!>\defgroup GFS_ozphys GFS ozphys Main +!! \brief This is the main subroutine !! \section arg_table_ozphys_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|---------------------------------------------------|---------------------------------------------------|---------|------|---------|-----------|--------|----------| @@ -78,22 +76,6 @@ end subroutine ozphys_init !! | ozp | change_in_ozone_concentration | change in ozone concentration | kg kg-1 | 3 | real | kind_phys | inout | F | !! | me | mpi_rank | rank of the current MPI task | index | 0 | integer | default | in | F | !! -!! \param[in] ix,im integer, horizontal dimension and num of used pts -!! \param[in] levs integer, vertical layer dimension -!! \param[in] ko3 integer, number of layers for ozone data -!! \param[in] dt real, physics time step in seconds -!! \param[in] ozi real, updated ozone -!! \param[out] ozo real, updated ozone -!! \param[in] tin real, updated temperature -!! \param[in] po3 real, (ko3), ozone forcing data level pressure -!! (ln(Pa)) -!! \param[in] prsl real, (ix,levs),mean layer pressure -!! \param[in] prdout real, (ix,ko3,pl_coeff),ozone forcing data -!! \param[in] pl_coeff integer, number coefficients in ozone forcing -!! \param[in] delp real, (ix,levs) -!! \param[in] ldiag3d logical, flag for 3d diagnostic fields -!! \param[out] ozp real, ozone change due to physics -!! \param[in] me integer, pe number - used for debug prints !! \section gen_al General Algorithm !> @{ subroutine ozphys_run ( & @@ -218,10 +200,9 @@ end subroutine ozphys_run !! @} !> @} -!> \ingroup GFS_ozphys -!! \brief Brief description of the subroutine -!! -!! \section arg_table_ozphys_finalize Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_ozphys_finalize Argument Table !! subroutine ozphys_finalize() end subroutine ozphys_finalize @@ -236,8 +217,8 @@ module ozphys_post contains -!! \section arg_table_ozphys_post_init Argument Table -!! +! \section arg_table_ozphys_post_init Argument Table +! subroutine ozphys_post_init() end subroutine ozphys_post_init @@ -272,8 +253,8 @@ subroutine ozphys_post_run(ix, levs, pl_coeff, ozp, Diag) end subroutine ozphys_post_run -!! \section arg_table_ozphys_post_finalize Argument Table -!! +! \section arg_table_ozphys_post_finalize Argument Table +! subroutine ozphys_post_finalize() end subroutine ozphys_post_finalize diff --git a/physics/precpd.f b/physics/precpd.f index fe3b9ee45..dd21c535d 100644 --- a/physics/precpd.f +++ b/physics/precpd.f @@ -9,16 +9,15 @@ module GFS_zhaocarr_precpd !> \defgroup precip Precipitation (snow or rain) Production !! @{ -!> \ingroup precip -!! \brief Brief description of the subroutine -!! -!! \section arg_table_precpd_init Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_precpd_init Argument Table +! subroutine precpd_init () end subroutine precpd_init -!> \ingroup precip +!> \defgroup gfs_precpd GFS precpd Main !! \brief This subroutine computes the conversion from condensation to !! precipitation (snow or rain) or evaporation of rain. !! @@ -739,11 +738,10 @@ subroutine precpd_run (im,ix,km,dt,del,prsl,q,cwm,t,rn,sr & end subroutine precpd_run !> @} -!> \ingroup precip -!! \brief Brief description of the subroutine -!! -!! \section arg_table_precpd_finalize Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_precpd_finalize Argument Table +! subroutine precpd_finalize end subroutine precpd_finalize diff --git a/physics/radlw_main.f b/physics/radlw_main.f index 456a9fdab..04abd2c1f 100644 --- a/physics/radlw_main.f +++ b/physics/radlw_main.f @@ -340,7 +340,7 @@ !! - radlw_main.f, which contains: !! - module_radlw_main, which is the main LW radiation transfer !! program and contains two externally callable subroutines: -!! - lwrad(): the main LW radiation routine +!! - lwrad_run(): the main LW radiation routine !! - rlwinit(): the initialization routine !! !! All the LW radiation subprograms become contained subprograms in @@ -478,68 +478,10 @@ module module_radlw_main ! contains ! ================ -!> This subroutine is the main LW radiation routine. -!!\param plyr model layer mean pressure in mb -!!\param plvl model interface pressure in mb -!!\param tlyr model layer mean temperature in K -!!\param tlvl model interface temperature in K -!!\param qlyr layer specific humidity in gm/gm -!!\param olyr layer ozone concentration in gm/gm -!!\param gasvmr atmospheric gases amount: -!!\n (:,:,1) - co2 volume mixing ratio -!!\n (:,:,2) - n2o volume mixing ratio -!!\n (:,:,3) - ch4 volume mixing ratio -!!\n (:,:,4) - o2 volume mixing ratio -!!\n (:,:,5) - co volume mixing ratio -!!\n (:,:,6) - cfc11 volume mixing ratio -!!\n (:,:,7) - cfc12 volume mixing ratio -!!\n (:,:,8) - cfc22 volume mixing ratio -!!\n (:,:,9) - ccl4 volume mixing ratio -!!\param clouds layer cloud profile -!!\n for ilwcliq > 0 --- -!!\n (:,:,1) - layer total cloud fraction -!!\n (:,:,2) - layer in-cloud liq water path (\f$ g/m^2 \f$) -!!\n (:,:,3) - mean eff radius for liq cloud (micron) -!!\n (:,:,4) - layer in-cloud ice water path (\f$ g/m^2 \f$) -!!\n (:,:,5) - mean eff radius for ice cloud (micron) -!!\n (:,:,6) - layer rain drop water path (\f$ g/m^2 \f$) -!!\n (:,:,7) - mean eff radius for rain drop (micron) -!!\n (:,:,8) - layer snow flake water path (\f$ g/m^2 \f$) -!!\n (:,:,9) - mean eff radius for snow flake(micron) -!!\n for ilwcliq = 0 --- -!!\n (:,:,1) - layer total cloud fraction -!!\n (:,:,2) - layer cloud optical depth -!!\n (:,:,3) - layer cloud single scattering albedo -!!\n (:,:,4) - layer cloud asymmetry factor -!!\param icseed auxiliary special cloud related array. -!!\param aerosols aerosol optical properties -!!\n (:,:,:,1) - optical depth -!!\n (:,:,:,2) - single scattering albedo -!!\n (:,:,:,3) - asymmetry parameter -!!\param sfemis surface emissivity -!!\param sfgtmp surface ground temperature in K -!!\param npts total number of horizontal points -!!\param nlay, nlp1 total number of vertical layers, levels -!!\param lprnt cntl flag for diagnostic print out -!!\param hlwc total sky heating rate in k/day or k/sec -!!\param topflx radiation fluxes at top, components -!!\n upfxc - total sky upward flux at top (\f$ w/m^2 \f$) -!!\n upfx0 - clear sky upward flux at top (\f$ w/m^2 \f$) -!!\param sfcflx radiation fluxes at sfc, components -!!\n upfxc - total sky upward flux at sfc (\f$ w/m^2 \f$) -!!\n dnfxc - total sky downward flux at sfc (\f$ w/m^2 \f$) -!!\n upfx0 - clear sky upward flux at sfc (\f$ w/m^2 \f$) -!!\n dnfx0 - clear sky downward flux at sfc (\f$ w/m^2 \f$) -!!\param hlwb spectral band total sky heating rates -!!\param hlw0 clear sky heating rates (k/sec or k/day) -!!\param flxprf level radiation fluxes (\f$ w/m^2 \f$), components -!!\n dnfxc - total sky downward flux -!!\n upfxc - total sky upward flux -!!\n dnfx0 - clear sky downward flux -!!\n upfx0 - clear sky upward flux subroutine lwrad_init () end subroutine lwrad_init +!> This subroutine is the main LW radiation routine. !! \section arg_table_lwrad_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |-----------------|----------------------------------------------------------------------------------------------|------------------------------------------------------------|---------|------|-------------|-----------|--------|----------| @@ -1405,7 +1347,6 @@ subroutine lwrad_finalize () end subroutine lwrad_finalize - !> This subroutine performs calculations necessary for the initialization !! of the longwave model. lookup tables are computed for use in the lw !! radiative transfer, and input absorption coefficient data for each diff --git a/physics/radsw_main.f b/physics/radsw_main.f index 0d50bc3b8..253494d42 100644 --- a/physics/radsw_main.f +++ b/physics/radsw_main.f @@ -511,79 +511,11 @@ module module_radsw_main ! contains ! ================= -!> This subroutine is the main SW radiation routine. -!!\param plyr model layer mean pressure in mb -!!\param plvl model level pressure in mb -!!\param tlyr model layer mean temperature in K -!!\param tlvl model level temperature in K (not in use) -!!\param qlyr layer specific humidity in gm/gm -!!\param olyr layer ozone concentration in gm/gm -!!\param gasvmr atmospheric constent gases -!!\n (:,:,1) - co2 volume mixing ratio -!!\n (:,:,2) - n2o volume mixing ratio -!!\n (:,:,3) - ch4 volume mixing ratio -!!\n (:,:,4) - o2 volume mixing ratio -!!\n (:,:,5) - co volume mixing ratio (not used) -!!\n (:,:,6) - cfc11 volume mixing ratio (not used) -!!\n (:,:,7) - cfc12 volume mixing ratio (not used) -!!\n (:,:,8) - cfc22 volume mixing ratio (not used) -!!\n (:,:,9) - ccl4 volume mixing ratio (not used) -!!\param clouds cloud profile -!!\n (:,:,1) - layer total cloud fraction -!!\n (:,:,2) - layer in-cloud liq water path (\f$g/m^2\f$) -!!\n (:,:,3) - mean eff radius for liq cloud (micron) -!!\n (:,:,4) - layer in-cloud ice water path (\f$g/m^2\f$) -!!\n (:,:,5) - mean eff radius for ice cloud (micron) -!!\n (:,:,6) - layer rain drop water path (\f$g/m^2\f$) -!!\n (:,:,7) - mean eff radius for rain drop (micron) -!!\n (:,:,8) - layer snow flake water path (\f$g/m^2\f$) -!!\n (:,:,9) - mean eff radius for snow flake (micron) -!!\param icseed auxiliary special cloud related array. -!!\param aerosols aerosol optical properties -!!\n (:,:,:,1) - optical depth -!!\n (:,:,:,2) - single scattering albedo -!!\n (:,:,:,3) - asymmetry parameter -!!\param sfcalb surface albedo in fraction -!!\n (:,1) - near ir direct beam albedo -!!\n (:,2) - near ir diffused albedo -!!\n (:,3) - uv+vis direct beam albedo -!!\n (:,4) - uv+vis diffused albedo -!!\param cosz cosine of solar zenith angle -!!\param solcon solar constant (\f$W/m^2\f$) -!!\param NDAY num of daytime points -!!\param idxday index array for daytime points -!!\param npts number of horizontal points -!!\param nlay,nlp1 vertical layer/lavel numbers -!!\param lprnt logical check print flag -!!\param hswc total sky heating rates (k/sec or k/day) -!!\param topflx radiation fluxes at toa (\f$W/m^2\f$), components: -!!\n upfxc - total sky upward flux at toa -!!\n dnflx - total sky downward flux at toa -!!\n upfx0 - clear sky upward flux at toa -!!\param sfcflx radiation fluxes at sfc (\f$W/m^2\f$), components: -!!\n upfxc - total sky upward flux at sfc -!!\n dnfxc - total sky downward flux at sfc -!!\n upfx0 - clear sky upward flux at sfc -!!\n dnfx0 - clear sky downward flux at sfc -!!\param hswb spectral band total sky heating rates -!!\param hsw0 clear sky heating rates (k/sec or k/day) -!!\param flxprf level radiation fluxes (\f$ W/m^2 \f$), components: -!!\n dnfxc - total sky downward flux at interface -!!\n upfxc - total sky upward flux at interface -!!\n dnfx0 - clear sky downward flux at interface -!!\n upfx0 - clear sky upward flux at interface -!!\param fdncmp surface downward fluxes (\f$W/m^2\f$), components: -!!\n uvbfc - total sky downward uv-b flux at sfc -!!\n uvbf0 - clear sky downward uv-b flux at sfc -!!\n nirbm - downward surface nir direct beam flux -!!\n nirdf - downward surface nir diffused flux -!!\n visbm - downward surface uv+vis direct beam flux -!!\n visdf - downward surface uv+vis diffused flux subroutine swrad_init () end subroutine swrad_init - +!>/brief This subroutine is the main SW radiation routine. !! \section arg_table_swrad_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |-----------------|-----------------------------------------------------------------------------------------------|--------------------------------------------------------------------------|---------|------|-------------|-----------|--------|----------| diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index 24b50fb50..822c1ac26 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -1,7 +1,7 @@ !> \file sfc_diff.f !! This file contains the surface exchange coefficient calculation scheme. -!> \defgroup Sfc_ex_cal Surface Exchange Coefficient Calculation +!> \defgroup Sfc_ex_cal GFS Surface Exchange Coefficient Calculation !! @{ !! \brief Brief description of the scheme !! \section diagram Calling Hierarchy Diagram @@ -17,8 +17,10 @@ subroutine sfc_ex_coef_finalize end subroutine sfc_ex_coef_finalize ! subroutine sfc_diff(im,ps,u1,v1,t1,q1,z1, + +!> \defgroup GFS_diff_main GFS sfc_diff Main +!! \ingroup Sfc_ex_cal !> \brief Brief description of the subroutine -!! !! \section arg_table_sfc_ex_coef_run Arguments !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|-------------------------------------------------|------------|------|---------|-----------|--------|----------| diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index 179cb7618..8d5e874ad 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -1,11 +1,11 @@ !> \file sfc_drv.f !! This file contains the NOAH land surface scheme. -!> \defgroup NOAH NOAH Land Surface Scheme +!> \defgroup NOAH GFS NOAH Land Surface Scheme !! \brief This is the NOAH land surface scheme. !! @{ -!> \defgroup NOAH_pre NOAH Land Surface Pre -!! \ingroup NOAH +! \defgroup NOAH_pre NOAH Land Surface Pre +! \ingroup NOAH !! @{ !! \brief Brief description of the parameterization @@ -18,9 +18,9 @@ end subroutine lsm_noah_pre_init subroutine lsm_noah_pre_finalize end subroutine lsm_noah_pre_finalize -!> \brief Brief description of the subroutine -!! -!! \section arg_table_lsm_noah_pre_run Arguments +! \brief Brief description of the subroutine +! +! \section arg_table_lsm_noah_pre_run Arguments !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|--------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -70,8 +70,8 @@ end module lsm_noah_pre !! @} -!> \defgroup NOAH_post NOAH Land Surface post -!! \ingroup NOAH +! \defgroup NOAH_post NOAH Land Surface post +! \ingroup NOAH !! @{ !! \brief Brief description of the parameterization !! \section diagram Calling Hierarchy Diagram @@ -86,9 +86,9 @@ end subroutine lsm_noah_post_init subroutine lsm_noah_post_finalize end subroutine lsm_noah_post_finalize -!> \brief Brief description of the subroutine -!! -!! \section arg_table_lsm_noah_post_run Arguments +! \brief Brief description of the subroutine +! +! \section arg_table_lsm_noah_post_run Arguments !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|--------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -132,13 +132,6 @@ end subroutine lsm_noah_post_run end module lsm_noah_post !! @} -!> \defgroup NOAH_main NOAH Land Surface Main -!! \ingroup NOAH -!! @{ -!! \brief Brief description of the parameterization -!! \section diagram Calling Hierarchy Diagram -!! \section intraphysics Intraphysics Communication - module lsm_noah contains @@ -255,6 +248,13 @@ end subroutine lsm_noah_finalize !----------------------------------- ! subroutine sfc_drv & +!> \defgroup NOAH_main GFS sfc_drv Main +!! \ingroup NOAH +!! @{ +!! \brief Brief description of the parameterization +!! \section diagram Calling Hierarchy Diagram +!! \section intraphysics Intraphysics Communication + !> \brief Brief description of the subroutine !! !! \section arg_table_lsm_noah_run Arguments diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index 6fe0531bb..2b314e4b7 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -1,12 +1,12 @@ !> \file sfc_nst.f !! This file contains the GFS NSST model. +!> \defgroup GFS_NSST GFS Near Sea Surface Temperature +!! @{ module sfc_nst contains -!> \defgroup GFS_NSST GFS Near Sea Surface Temperature -!! @{ !! \brief Near Sea Surface Temperature (NSST) is a temperature profile just below the sea surface. The GFS NSST scheme is used to forecast the NSST for two main purposes: supply SSTs to the atmospheric model for the calculation of air-sea heat and moisture fluxes and providing a sub-layer temperature profile forecast for use as a first guess in the Gridpoint Statistical Interpolator (GSI) data assimilation code. !! !! The GFS NSST scheme was initially developed at NCEP by Xu Li in 2007, and subsequently received contributions by S. Moorthi, Y.-T. Hu and J. Derber, leading to operational implementation in the GFS in 2017 (Li 2015 \cite Li_2015, and Li and Derber 2009 \cite Li_Derber_2009). The GFS NSST scheme predicts the vertical profile of sea temperature between the surface and a reference level (zr), which is on the order of 5 m. Only two physical process are considered in this scheme: diurnal thermocline layer warming and thermal skin layer (also known as sub-layer) cooling. All other process that could influence NSST are ignored in this simple scheme. @@ -32,8 +32,7 @@ module sfc_nst !! !! This space is reserved for a description of how this scheme uses information from other scheme types and/or how information calculated in this scheme is used in other scheme types. -!> \brief This subroutine is empty since there are no procedures that need to be done to initialize the GFS NSST code. -!! +! \brief This subroutine is empty since there are no procedures that need to be done to initialize the GFS NSST code. !! This subroutine is empty since there are no procedures that need to be done to initialize the GFS NSST code. !! !! \section arg_table_sfc_nst_init Argument Table @@ -41,19 +40,16 @@ module sfc_nst subroutine sfc_nst_init end subroutine sfc_nst_init -!> \brief This subroutine is empty since there are no procedures that need to be done to finalize the GFS NSST code. -!! +! \brief This subroutine is empty since there are no procedures that need to be done to finalize the GFS NSST code. !! This subroutine is empty since there are no procedures that need to be done to finalize the GFS NSST code. -!! !! \section arg_table_sfc_nst_finalize Argument Table !! subroutine sfc_nst_finalize end subroutine sfc_nst_finalize +!>\defgroup gfs_nst_main GFS sfc_nst Main !> \brief This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. -!! !! This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. -!! !! \section arg_table_sfc_nst_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------------|-------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| @@ -703,7 +699,7 @@ module sfc_nst_pre contains -!> \defgroup GFS_NSST_PRE GFS Near Sea Surface Temperature Pre +! \defgroup GFS_NSST_PRE GFS Near Sea Surface Temperature Pre !! @{ !! \brief Brief description of the parameterization !! @@ -804,7 +800,7 @@ module sfc_nst_post contains -!> \defgroup GFS_NSST_POST GFS Near Sea Surface Temperature Post +! \defgroup GFS_NSST_POST GFS Near Sea Surface Temperature Post !! @{ !! \brief Brief description of the parameterization !! diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 9008989af..cf0735b05 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -1,12 +1,11 @@ !> \file sfc_sice.f !! This file contains the GFS three level thermodynamic sea ice model. +!> \defgroup GFS_Ice GFS Thermodynamics Sea Ice module sfc_sice contains -!> \defgroup GFS_Ice GFS Thermodynamics Sea Ice -!! @{ !! \brief Three layer thermodynamic sea ice model based on M. Winton's "a reformulated three-layer sea ice model", journal of atmospheric and oceanic technology, 2000. !! \section diagram Calling Hierarchy Diagram !! \section intraphysics Intraphysics Communication @@ -22,7 +21,12 @@ end subroutine sfc_sice_init !! subroutine sfc_sice_finalize end subroutine sfc_sice_finalize -!! + + +!>\defgroup gfs_sice_main GFS sfc_sice Main +!> \brief blah blah +!! @{ +!! \ingroup GFS_Ice !! \section arg_table_sfc_sice_run Arguments !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------------|-----------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| @@ -97,7 +101,7 @@ subroutine sfc_sice_run & ! ! ! subprogram called: ice3lay. ! ! ! -! program history log: ! +u program history log: ! ! 2005 -- xingren wu created from original progtm and added ! ! two-layer ice model ! ! 200x -- sarah lu added flag_iter ! @@ -728,21 +732,20 @@ module sfc_sice_pre contains !! -!> \brief This subroutine is empty since there are no procedures needed -!! \section arg_table_sfc_sice_pre_init Argument Table +! \brief This subroutine is empty since there are no procedures needed +! \section arg_table_sfc_sice_pre_init Argument Table !! subroutine sfc_sice_pre_init end subroutine sfc_sice_pre_init !! -!> \brief This subroutine is empty since there are no procedures needed -!! \section arg_table_sfc_sice_pre_finalize Argument Table +! \brief This subroutine is empty since there are no procedures needed +! \section arg_table_sfc_sice_pre_finalize Argument Table !! subroutine sfc_sice_pre_finalize end subroutine sfc_sice_pre_finalize -!! !! \section arg_table_sfc_sice_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------------|-------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| @@ -795,15 +798,15 @@ module sfc_sice_post contains !! -!> \brief This subroutine is empty since there are no procedures needed -!! \section arg_table_sfc_sice_post_init Argument Table +! \brief This subroutine is empty since there are no procedures needed +! \section arg_table_sfc_sice_post_init Argument Table !! subroutine sfc_sice_post_init end subroutine sfc_sice_post_init !! -!> \brief This subroutine is empty since there are no procedures needed -!! \section arg_table_sfc_sice_post_finalize Argument Table +! \brief This subroutine is empty since there are no procedures needed +! \section arg_table_sfc_sice_post_finalize Argument Table !! subroutine sfc_sice_post_finalize end subroutine sfc_sice_post_finalize @@ -860,6 +863,7 @@ subroutine sfc_sice_post_run(im, islmsk, cice, zice, tice, tsfc, & enddo end subroutine sfc_sice_post_run +!! @} end module sfc_sice_post !> @} From d06a3c2e473c7be147774572fe15d233b126f205 Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Tue, 23 Jan 2018 17:00:23 -0700 Subject: [PATCH 04/22] add mfshalcnv documentation and clean up in other files. --- physics/mfshalcnv.f | 192 ++++++++++++++++++++++++++++++++-- physics/radiation_aerosols.f | 178 +++++++++++++++---------------- physics/radiation_astronomy.f | 18 ++-- physics/radiation_clouds.f | 61 +++++------ physics/radiation_gases.f | 34 +++--- physics/radiation_surface.f | 10 +- physics/radlw_datatb.f | 40 +++---- physics/radlw_main.f | 18 ++-- physics/radlw_param.f | 54 +++++----- physics/radsw_datatb.f | 37 +++---- physics/radsw_main.f | 36 +++---- physics/radsw_param.f | 75 ++++++------- physics/sfc_drv.f | 22 ++-- physics/sfc_nst.f | 15 ++- physics/sfc_sice.f | 13 ++- 15 files changed, 486 insertions(+), 317 deletions(-) diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 80892c309..b141faf3e 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -233,6 +233,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! !************************************************************************ ! convert input Pa terms to Cb terms -- Moorthi +!> ## Compute preliminary quantities needed for the static and feedback control portions of the algorithm. +!> - Convert input pressure terms to centibar units. ps = psp * 0.001 prsl = prslp * 0.001 del = delp * 0.001 @@ -242,6 +244,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c initialize arrays c +!> - Initialize column-integrated and other single-value-per-column variable arrays. do i=1,im cnvflg(i) = .true. if(kcnv(i) == 1) cnvflg(i) = .false. @@ -263,12 +266,14 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & gdx(i) = sqrt(garea(i)) enddo !! +!> - Return to the calling routine if deep convection is present or the surface buoyancy flux is negative. totflg = .true. do i=1,im totflg = totflg .and. (.not. cnvflg(i)) enddo if(totflg) return !! +!> - determine aerosol-aware rain conversion parameter over land do i=1,im if(islimsk(i) == 1) then c0(i) = c0l @@ -277,6 +282,9 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo ! +!> - determine rain conversion parameter above the freezing level +!! which exponentially decreases with decreasing temperature from +!! Han et al.'s (2017) \cite han_et_al_2017 equation 8. do k = 1, km do i = 1, im if(t1(i,k) > 273.16) then @@ -289,6 +297,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo ! +!> - Initialize convective cloud water and cloud cover to zero. do k = 1, km do i = 1, im cnvw(i,k) = 0. @@ -296,6 +305,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo ! hchuang code change +!> - Initialize updraft mass fluxes to zero. do k = 1, km do i = 1, im ud_mf(i,k) = 0. @@ -326,6 +336,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c define top layer for search of the downdraft originating layer c and the maximum thetae for updraft c +!> - Determine maximum indices for the parcel starting point (kbm) and cloud top (kmax). do i=1,im kbm(i) = km kmax(i) = km @@ -345,11 +356,15 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c hydrostatic height assume zero terr and compute c updraft entrainment rate as an inverse function of height c +!> - Calculate hydrostatic height at layer centers assuming a flat +!! surface (no terrain) from the geopotential. do k = 1, km do i=1,im zo(i,k) = phil(i,k) / g enddo enddo +!> - Calculate interface height and the entrainment rate as an inverse +!! function of height. do k = 1, km1 do i=1,im zi(i,k) = 0.5*(zo(i,k)+zo(i,k+1)) @@ -362,6 +377,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c pbl height c +!> - Find the index for the PBL top using the PBL height; enforce that +!! it is lower than the maximum parcel starting level. do i=1,im flg(i) = cnvflg(i) kpbl(i)= 1 @@ -382,6 +399,9 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! c convert surface pressure to mb from cb c +!> - Convert prsl from centibar to millibar, set normalized mass flux +!! to 1, cloud properties to 0, and save model state variables (after +!! advection/turbulence). do k = 1, km do i = 1, im if (cnvflg(i) .and. k <= kmax(i)) then @@ -416,6 +436,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c to is temperature at t+dt (k)... this is after advection and turbulence c qo is specific humidity at t+dt (kg/kg)..q1 c +!> - Calculate saturation specific humidity and enforce minimum moisture values. do k = 1, km do i=1,im if (cnvflg(i) .and. k <= kmax(i)) then @@ -433,6 +454,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c compute moist static energy c +!> - Calculate moist static energy (heo) and saturation moist static energy (heso). do k = 1, km do i=1,im if (cnvflg(i) .and. k <= kmax(i)) then @@ -448,6 +470,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c determine level with largest moist static energy within pbl c this is the level where updraft starts c +!> ## Perform calculations related to the updraft of the entraining/detraining cloud model ("static control"). +!> - Search in the PBL for the level of maximum moist static energy to start the ascending parcel. do i=1,im if (cnvflg(i)) then hmax(i) = heo(i,1) @@ -465,6 +489,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo c +!> - Calculate the temperature, water vapor mixing ratio, and pressure at interface levels. do k = 1, km1 do i=1,im if (cnvflg(i) .and. k <= kmax(i)-1) then @@ -486,6 +511,9 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo ! +!> - Recalculate saturation specific humidity, moist static energy, +!! saturation moist static energy, and horizontal momentum on interface +!! levels. Enforce minimum specific humidity. do k = 1, km1 do i=1,im if (cnvflg(i) .and. k <= kmax(i)-1) then @@ -508,6 +536,11 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c look for the level of free convection as cloud base c +!> - Search below the index "kbm" for the level of free convection (LFC) +!! where the condition \f$h_b > h^*\f$ is first met, where \f$h_b, h^*\f$ +!! are the state moist static energy at the parcel's starting level and +!! saturation moist static energy, respectively. Set "kbcon" to the +!! index of the LFC. do i=1,im flg(i) = cnvflg(i) if(flg(i)) kbcon(i) = kmax(i) @@ -529,12 +562,20 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo !! +!> - If no LFC, return to the calling routine without modifying state variables. totflg = .true. do i=1,im totflg = totflg .and. (.not. cnvflg(i)) enddo if(totflg) return !! +!> - Determine the vertical pressure velocity at the LFC. After Han and +!! Pan (2011) \cite han_and_pan_2011 , determine the maximum pressure +!! thickness between a parcel's starting level and the LFC. If a parcel +!! doesn't reach the LFC within the critical thickness, then the convective +!! inhibition is deemed too great for convection to be triggered, and the +!! subroutine returns to the calling routine without modifying the state +!! variables. do i=1,im if(cnvflg(i)) then ! pdot(i) = 10.* dot(i,kbcon(i)) @@ -588,6 +629,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c specify the detrainment rate for the updrafts c +!> - The updraft detrainment rate is set constant and equal to the entrainment rate at cloud base. do i = 1, im if(cnvflg(i)) then xlamud(i) = xlamue(i,kbcon(i)) @@ -597,6 +639,15 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c determine updraft mass flux for the subcloud layers c +!> - Calculate the normalized mass flux for subcloud and in-cloud layers +!! according to Pan and Wu (1995) \cite pan_and_wu_1995 equation 1: +!! \f[ +!! \frac{1}{\eta}\frac{\partial \eta}{\partial z} = \lambda_e - \lambda_d +!! \f] +!! where \f$\eta\f$ is the normalized mass flux, \f$\lambda_e\f$ is the +!! entrainment rate and \f$\lambda_d\f$ is the detrainment rate. The +!! normalized mass flux increases upward below the cloud base and decreases +!! upward above. do k = km1, 1, -1 do i = 1, im if (cnvflg(i)) then @@ -634,6 +685,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c compute updraft cloud property c +!> - Set cloud properties equal to the state variables at updraft starting level (kb). do i = 1, im if(cnvflg(i)) then indx = kb(i) @@ -645,6 +697,13 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c ! cm is an enhancement factor in entrainment rates for momentum ! +!> - Calculate the cloud properties as a parcel ascends, modified by +!! entrainment and detrainment. Discretization follows Appendix B of +!! Grell (1993) \cite grell_1993 . Following Han and Pan (2006) +!! \cite han_and_pan_2006, the convective momentum transport is reduced +!! by the convection-induced pressure gradient force by the constant +!! "pgcon", currently set to 0.55 after Zhang and Wu (2003) +!! \cite zhang_and_wu_2003 . do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -673,6 +732,13 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c taking account into convection inhibition due to existence of c dry layers below cloud base c +!> - With entrainment, recalculate the LFC as the first level where +!! buoyancy is positive. The difference in pressure levels between LFCs +!! calculated with/without entrainment must be less than a threshold +!! (currently 25 hPa). Otherwise, convection is inhibited and the scheme +!! returns to the calling routine without modifying the state variables. +!! This is the subcloud dryness trigger modification discussed in Han +!! and Pan (2011) \cite han_and_pan_2011. do i=1,im flg(i) = cnvflg(i) kbcon1(i) = kmax(i) @@ -710,6 +776,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c calculate convective inhibition c +!> - Calculate additional trigger condition of the convective inhibition +!! (CIN) according to Han et al.'s (2017) \cite han_et_al_2017 equation 13. do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -732,6 +800,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo +!> - Turn off convection if the CIN is less than a critical value (cinacr) +!! which is inversely proportional to the large-scale vertical velocity. do i = 1, im if(cnvflg(i)) then ! @@ -777,6 +847,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c determine first guess cloud top as the level of zero buoyancy c limited to the level of P/Ps=0.7 c +!> - Calculate the cloud top as the first level where parcel buoyancy +!! becomes negative; the maximum possible value is at \f$p=0.7p_{sfc}\f$. do i = 1, im flg(i) = cnvflg(i) if(flg(i)) ktcon(i) = kbm(i) @@ -794,6 +866,9 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c specify upper limit of mass flux at cloud base c +!> - Calculate the maximum value of the cloud base mass flux using the +!! CFL-criterion-based formula of Han and Pan (2011) \cite han_and_pan_2011, +!! equation 7. do i = 1, im if(cnvflg(i)) then ! xmbmax(i) = .1 @@ -809,6 +884,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c compute cloud moisture property and precipitation c +!> - Set cloud moisture property equal to the enviromental moisture at +!! updraft starting level (kb). do i = 1, im if (cnvflg(i)) then aa1(i) = 0. @@ -816,6 +893,16 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & qrcko(i,kb(i)) = qo(i,kb(i)) endif enddo +!> - Calculate the moisture content of the entraining/detraining parcel +!! (qcko) and the value it would have if just saturated (qrch), according +!! to equation A.14 in Grell (1993) \cite grell_1993 . Their difference +!! is the amount of convective cloud water (qlk = rain + condensate). +!! Determine the portion of convective cloud water that remains suspended +!! and the portion that is converted into convective precipitation (pwo). +!! Calculate and save the negative cloud work function (aa1) due to water +!! loading. Above the level of minimum moist static energy, some of the +!! cloud water is detrained into the grid-scale cloud water from every +!! cloud layer with a rate of 0.0005 \f$m^{-1}\f$ (dellal). do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -903,6 +990,18 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! ! calculate cloud work function ! +!> - Calculate the cloud work function according to Pan and Wu (1995) +!! \cite pan_and_wu_1995 equation 4: +!! \f[ +!! A_u=\int_{z_0}^{z_t}\frac{g}{c_pT(z)}\frac{\eta}{1 + \gamma}[h(z)-h^*(z)]dz +!! \f] +!! (discretized according to Grell (1993) \cite grell_1993 equation B.10 +!! using B.2 and B.3 of Arakawa and Schubert (1974) \cite arakawa_and_schubert_1974 +!! and assuming \f$\eta=1\f$) where \f$A_u\f$ is the updraft cloud work function, +!! \f$z_0\f$ and \f$z_t\f$ are cloud base and cloud top, respectively, +!! \f$\gamma = \frac{L}{c_p}\left(\frac{\partial \overline{q_s}}{\partial T}\right)_p\f$ +!! and other quantities are previously defined. + do i = 1, im do i = 1, im if (cnvflg(i)) then aa1(i) = 0. @@ -922,6 +1021,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & if(cnvflg(i) .and. aa1(i) <= 0.) cnvflg(i) = .false. enddo !! +!> - If the updraft cloud work function is negative, convection does not +!! occur, and the scheme returns to the calling routine. totflg = .true. do i=1,im totflg = totflg .and. (.not. cnvflg(i)) @@ -934,6 +1035,12 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c which is the final cloud top c limited to the level of P/Ps=0.7 c +!> - Continue calculating the cloud work function past the point of +!! neutral buoyancy to represent overshooting according to Han and Pan +!! (2011) \cite han_and_pan_2011 . Convective overshooting stops when +!! \f$ cA_u < 0\f$ where \f$c\f$ is currently 10%, or when 10% of the +!! updraft cloud work function has been consumed by the stable buoyancy +!! force. Overshooting is also limited to the level where \f$p=0.7p_{sfc}\f$. do i = 1, im if (cnvflg(i)) then aa1(i) = aafac * aa1(i) @@ -974,6 +1081,10 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c compute cloud moisture property, detraining cloud water c and precipitation in overshooting layers c +!> - For the overshooting convection, calculate the moisture content of +!! the entraining/detraining parcel as before. Partition convective cloud +!! water and precipitation and detrain convective cloud water in the +!! overshooting layers. do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -1014,6 +1125,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo ! ! compute updraft velocity square(wu2) +!> - Calculate updraft velocity square(wu2) according to Han et al.'s +!! (2017) \cite han_et_al_2017 equation 7. ! ! bb1 = 2. * (1.+bet1*cd1) ! bb2 = 2. / (f1*(1.+gam1)) @@ -1057,6 +1170,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! ! compute updraft velocity averaged over the whole cumulus ! +!> - Calculate the mean updraft velocity within the cloud (wc). do i = 1, im wc(i) = 0. sumx(i) = 0. @@ -1101,6 +1215,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c compute liquid and vapor separation at cloud top c +!> - => Separate the total updraft cloud water at cloud top into vapor and condensate. do i = 1, im if(cnvflg(i)) then k = ktcon(i) - 1 @@ -1121,6 +1236,15 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c--- compute precipitation efficiency in terms of windshear c +!! - Calculate the wind shear and precipitation efficiency according to +!! equation 58 in Fritsch and Chappell (1980) \cite fritsch_and_chappell_1980 : +!! \f[ +!! E = 1.591 - 0.639\frac{\Delta V}{\Delta z} + 0.0953\left(\frac{\Delta V}{\Delta z}\right)^2 - 0.00496\left(\frac{\Delta V}{\Delta z}\right)^3 +!! \f] +!! where \f$\Delta V\f$ is the integrated horizontal shear over the cloud +!! depth, \f$\Delta z\f$, (the ratio is converted to units of +!! \f$10^{-3} s^{-1}\f$). The variable "edt" is \f$1-E\f$ and is +!! constrained to the range \f$[0,0.9]\f$. do i = 1, im if(cnvflg(i)) then vshear(i) = 0. @@ -1153,6 +1277,11 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c--- what would the change be, that a cloud with unit mass c--- will do to the environment? c +!> ## Calculate the tendencies of the state variables (per unit cloud base mass flux) and the cloud base mass flux. +!> - Calculate the change in moist static energy, moisture mixing ratio, +!! and horizontal winds per unit cloud base mass flux for all layers +!! below cloud top from equations B.14 and B.15 from Grell (1993) +!! \cite grell_1993, and for the cloud top from B.16 and B.17. do k = 1, km do i = 1, im if(cnvflg(i) .and. k <= kmax(i)) then @@ -1235,6 +1364,9 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! ! compute convective turn-over time ! +!> - Following Bechtold et al. (2008) \cite bechtold_et_al_2008, +!! calculate the convective turnover time using the mean updraft velocity +!! (wc) and the cloud depth. It is also proportional to the grid size (gdx). do i= 1, im if(cnvflg(i)) then tem = zi(i,ktcon1(i)) - zi(i,kbcon1(i)) @@ -1247,8 +1379,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo ! -! compute advective time scale using a mean cloud layer wind speed -! +!> - Calculate advective time scale (tauadv) using a mean cloud layer wind speed. do i= 1, im if(cnvflg(i)) then sumx(i) = 0. @@ -1278,6 +1409,12 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c compute cloud base mass flux as a function of the mean c updraft velcoity c +!> - From Han et al.'s (2017) \cite han_et_al_2017 equation 6, calculate cloud base mass flux as a function of the mean updraft velcoity. +!! As discussed in Han et al. (2017) \cite han_et_al_2017 , when dtconv +!! is larger than tauadv, the convective mixing is not fully conducted +!! before the cumulus cloud is advected out of the grid cell. In this +!! case, therefore, the cloud base mass flux is further reduced in +!! proportion to the ratio of tauadv to dtconv. do i= 1, im if(cnvflg(i)) then k = kbcon(i) @@ -1288,9 +1425,11 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo ! -!--- modified Grell & Freitas' (2014) updraft fraction which uses -! actual entrainment rate at cloud base -! +!> - For scale-aware parameterization, the updraft fraction (sigmagfm) +!! is first computed as a function of the lateral entrainment rate at +!! cloud base (see Han et al.'s (2017) \cite han_et_al_2017 equation 4 +!! and 5), following the study by Grell and Freitas (2014) +!! \cite grell_and_freitas_2014. do i = 1, im if(cnvflg(i)) then tem = min(max(xlamue(i,kbcon(i)), 2.e-4), 6.e-4) @@ -1302,9 +1441,13 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo ! -!--- compute scale-aware function based on Arakawa & Wu (2013) -! -! +!> - Then, calculate the reduction factor (scaldfunc) of the vertical +!! convective eddy transport of mass flux as a function of updraft +!! fraction from the studies by Arakawa and Wu (2013) \cite arakawa_and_wu_2013 +!! (also see Han et al.'s (2017) \cite han_et_al_2017 equation 1 and 2). +!! The final cloud base mass flux with scale-aware parameterization is +!! obtained from the mass flux when sigmagfm << 1, multiplied by the +!! reduction factor (Han et al.'s (2017) \cite han_et_al_2017 equation 2). do i = 1, im if(cnvflg(i)) then if (gdx(i) < dxcrt) then @@ -1317,6 +1460,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & xmb(i) = min(xmb(i),xmbmax(i)) endif enddo +!> ## For the "feedback control", calculate updated values of the state variables by multiplying the cloud base mass flux and the tendencies calculated per unit cloud base mass flux from the static control. +!! - Recalculate saturation specific humidity. c c!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! c @@ -1332,6 +1477,12 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo c!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! c +!> - Calculate the temperature tendency from the moist static energy and +!! specific humidity tendencies. +!> - Update the temperature, specific humidity, and horiztonal wind +!! state variables by multiplying the cloud base mass flux-normalized +!! tendencies by the cloud base mass flux. +!> - Accumulate column-integrated tendencies. do i = 1, im delhbar(i) = 0. delqbar(i) = 0. @@ -1363,6 +1514,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo ! +!> - Recalculate saturation specific humidity using the updated temperature. do k = 1, km do i = 1, im if (cnvflg(i)) then @@ -1376,6 +1528,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo enddo c +!> - Add up column-integrated convective precipitation by multiplying +!! the normalized value by the cloud base mass flux. do i = 1, im rntot(i) = 0. delqev(i) = 0. @@ -1394,6 +1548,12 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c evaporating rain c +!> - Determine the evaporation of the convective precipitation and +!! update the integrated convective precipitation. +!> - Update state temperature and moisture to account for evaporation +!! of convective precipitation. +!> - Update column-integrated tendencies to account for evaporation of +!! convective precipitation. do k = km, 1, -1 do i = 1, im if (k <= kmax(i)) then @@ -1467,6 +1627,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c convective cloud water c +!> - Calculate shallow convective cloud water. do k = 1, km do i = 1, im if (cnvflg(i)) then @@ -1480,6 +1641,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c convective cloud cover c +!> - Calculate convective cloud cover, which is used when pdf-based cloud +!! fraction is used (i.e., pdfcld=.true.). do k = 1, km do i = 1, im if (cnvflg(i)) then @@ -1495,6 +1658,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & c c cloud water c +!> - Separate detrained cloud water into liquid and ice species as a +!! function of temperature only. if (ncloud > 0) then ! do k = 1, km1 @@ -1519,6 +1684,10 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & ! ! hchuang code change ! +!> - Calculate and retain the updraft mass flux for dust transport by +!! cumulus convection. +! +!> - Calculate the updraft convective mass flux. do k = 1, km do i = 1, im if(cnvflg(i)) then @@ -1528,6 +1697,7 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & endif enddo enddo +!> - save the updraft convective mass flux at cloud top. do i = 1, im if(cnvflg(i)) then k = ktop(i)-1 @@ -1605,9 +1775,9 @@ subroutine sasasshal_post_run (frain, rain1, cnvc, cnvw, Model, & end subroutine sasasshal_post_run -!> \brief Brief description of the subroutine -!! -!! \section arg_table_sasasshal_post_init Argument Table +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_post_init Argument Table !! subroutine sasasshal_post_init () end subroutine sasasshal_post_init diff --git a/physics/radiation_aerosols.f b/physics/radiation_aerosols.f index 2572854d0..cf3dfbb52 100644 --- a/physics/radiation_aerosols.f +++ b/physics/radiation_aerosols.f @@ -167,28 +167,28 @@ module module_radiation_aerosols ! ! & VTAGAER='NCEP-Radiation_aerosols v5.0 Aug 2012 ' ! --- general use parameter constants: -!> num of output fields for SW rad +! num of output fields for SW rad integer, parameter, public :: NF_AESW = 3 -!> num of output fields for LW rad +! num of output fields for LW rad integer, parameter, public :: NF_AELW = 3 -!> starting band number in ir region +! starting band number in ir region integer, parameter, public :: NLWSTR = 1 -!> num of species for output aod (opnl) +! num of species for output aod (opnl) integer, parameter, public :: NSPC = 5 -!> total+species +! total+species integer, parameter, public :: NSPC1 = NSPC + 1 real (kind=kind_phys), parameter :: f_zero = 0.0 real (kind=kind_phys), parameter :: f_one = 1.0 ! --- module control parameters set in subroutine "aer_init" -!> number of actual bands for sw aerosols; calculated according to +! number of actual bands for sw aerosols; calculated according to !! laswflg setting integer, save :: NSWBND = NBDSW -!> number of actual bands for lw aerosols; calculated according to +! number of actual bands for lw aerosols; calculated according to !! lalwflg and lalw1bd settings integer, save :: NLWBND = NBDLW -!> total number of bands for sw+lw aerosols +! total number of bands for sw+lw aerosols integer, save :: NSWLWBD = NBDSW+NBDLW ! --------------------------------------------------------------------- ! @@ -197,15 +197,15 @@ module module_radiation_aerosols ! ! --------------------------------------------------------------------- ! ! --- parameter constants: -!> num of wvnum regions where solar flux is constant +! num of wvnum regions where solar flux is constant integer, parameter, public :: NWVSOL = 151 -!> total num of wvnum included +! total num of wvnum included integer, parameter, public :: NWVTOT = 57600 -!> total num of wvnum in ir range +! total num of wvnum in ir range integer, parameter, public :: NWVTIR = 4000 -!> number of wavenumbers in each region where the solar flux is constant +! number of wavenumbers in each region where the solar flux is constant integer, dimension(NWVSOL), save :: nwvns0 data nwvns0 / 100, 11, 14, 18, 24, 33, 50, 83, 12, 12, & @@ -221,7 +221,7 @@ module module_radiation_aerosols ! & 483, 505, 529, 554, 580, 610, 641, 675, 711, 751, 793, 841, 891, & & 947,1008,1075,1150,1231,1323,1425,1538,1667,1633,14300 / -!> solar flux \f$w/m^2\f$ in each wvnumb region where it is constant +! solar flux \f$w/m^2\f$ in each wvnumb region where it is constant real (kind=kind_phys), dimension(NWVSOL), save :: s0intv data s0intv( 1: 50) / & @@ -264,22 +264,22 @@ module module_radiation_aerosols ! ! --------------------------------------------------------------------- ! ! --- parameter constants: -!> lower limit (year) data available +! lower limit (year) data available integer, parameter :: MINVYR = 1850 -!> upper limit (year) data available +! upper limit (year) data available integer, parameter :: MAXVYR = 1999 -!> monthly, 45-deg lat-zone aerosols data set in subroutine 'aer_init' +! monthly, 45-deg lat-zone aerosols data set in subroutine 'aer_init' integer, allocatable, save :: ivolae(:,:,:) ! --- static control variables: -!> starting year of data in the input file +! starting year of data in the input file integer :: kyrstr -!> ending year of data in the input file +! ending year of data in the input file integer :: kyrend -!> the year of data in use in the input file +! the year of data in use in the input file integer :: kyrsav -!> the month of data in use in the input file +! the month of data in use in the input file integer :: kmonsav ! --------------------------------------------------------------------- ! @@ -288,27 +288,27 @@ module module_radiation_aerosols ! ! --------------------------------------------------------------------- ! ! --- parameters and constants: -!> num of max componets in a profile +! num of max componets in a profile integer, parameter :: NXC = 5 -!> num of aerosols profile structures +! num of aerosols profile structures integer, parameter :: NAE = 7 -!> num of atmos aerosols domains +! num of atmos aerosols domains integer, parameter :: NDM = 5 -!> num of lon-points in glb aeros data set +! num of lon-points in glb aeros data set integer, parameter :: IMXAE = 72 -!> num of lat-points in glb aeros data set +! num of lat-points in glb aeros data set integer, parameter :: JMXAE = 37 -!> num of bands for clim aer data (opac) +! num of bands for clim aer data (opac) integer, parameter :: NAERBND=61 -!> num of rh levels for rh-dep components +! num of rh levels for rh-dep components integer, parameter :: NRHLEV =8 -!> num of rh independent aeros species +! num of rh independent aeros species integer, parameter :: NCM1 = 6 -!> num of rh dependent aeros species +! num of rh dependent aeros species integer, parameter :: NCM2 = 4 integer, parameter :: NCM = NCM1+NCM2 -!> predefined relative humidity levels +! predefined relative humidity levels real (kind=kind_phys), dimension(NRHLEV), save :: rhlev data rhlev (:) / 0.0, 0.5, 0.7, 0.8, 0.9, 0.95, 0.98, 0.99 / @@ -319,11 +319,11 @@ module module_radiation_aerosols ! ! prsref(NDM,NAE) - ref pressure lev (sfc to toa) in mb (100Pa) ! sigref(NDM,NAE) - ref sigma lev (sfc to toa) -!> scale height of aerosols (km) +! scale height of aerosols (km) real (kind=kind_phys), save, dimension(NDM,NAE) :: haer -!> ref pressure lev (sfc to toa) in mb (100Pa) +! ref pressure lev (sfc to toa) in mb (100Pa) real (kind=kind_phys), save, dimension(NDM,NAE) :: prsref -!> ref sigma lev (sfc to toa) +! ref sigma lev (sfc to toa) real (kind=kind_phys), save, dimension(NDM,NAE) :: sigref ! --- the following arrays are allocate and setup in subr 'clim_aerinit' @@ -360,37 +360,37 @@ module module_radiation_aerosols ! ! cmixg (NXC*IMXAE*JMXAE) - aeros component mixing ratio ! denng ( 2 *IMXAE*JMXAE) - aerosols number density -!> \name topospheric aerosol profile distribution +! \name topospheric aerosol profile distribution -!> aeros component mixing ratio +! aeros component mixing ratio real (kind=kind_phys), dimension(NXC,IMXAE,JMXAE), save :: cmixg -!> aeros number density +! aeros number density real (kind=kind_phys), dimension( 2 ,IMXAE,JMXAE), save :: denng -!> aeros component index +! aeros component index integer, dimension(NXC,IMXAE,JMXAE), save :: idxcg -!> aeros profile index +! aeros profile index integer, dimension( IMXAE,JMXAE), save :: kprfg ! --------------------------------------------------------------------- ! ! section-4 : module variables for gocart aerosol optical properties ! ! --------------------------------------------------------------------- ! -!> \name module variables for gocart aerosol optical properties +! \name module variables for gocart aerosol optical properties ! --- parameters and constants: ! - KCM, KCM1, KCM2 are determined from subroutine 'set_aerspc' -!> num of bands for aer data (gocart) +! num of bands for aer data (gocart) integer, parameter :: KAERBND=61 -!> num of rh levels for rh-dep components +! num of rh levels for rh-dep components integer, parameter :: KRHLEV =36 !* integer, parameter :: KCM1 = 8 ! num of rh independent aer !species !* integer, parameter :: KCM2 = 5 ! num of rh dependent aer species !* integer, parameter :: KCM = KCM1 + KCM2 -!> num of rh indep aerosols (set in subr set_aerspc) +! num of rh indep aerosols (set in subr set_aerspc) integer, save :: KCM1 = 0 -!> num of rh dep aerosols (set in subr set_aerspc) +! num of rh dep aerosols (set in subr set_aerspc) integer, save :: KCM2 = 0 -!> =KCM1+KCM2 (set in subr set_aerspc) +! =KCM1+KCM2 (set in subr set_aerspc) integer, save :: KCM real (kind=kind_phys), dimension(KRHLEV) :: rhlev_grt & @@ -430,32 +430,32 @@ module module_radiation_aerosols ! ! rhdpssa0_grt(KAERBND,KRHLEV,KCM2) - single scattering albedo ! rhdpasy0_grt(KAERBND,KRHLEV,KCM2) - asymmetry parameter -!> spectral band structure: ending wavenumber (\f$cm^-1\f$) for each band +! spectral band structure: ending wavenumber (\f$cm^-1\f$) for each band integer, allocatable, dimension(:) :: iendwv_grt ! relative humidity independent aerosol optical properties: !! species : dust (8 bins) -!> \name relative humidity independent aerosol optical properties: -!! species : dust (8 bins) +! \name relative humidity independent aerosol optical properties: +! species : dust (8 bins) -!> extinction coefficient +! extinction coefficient real (kind=kind_phys),allocatable, dimension(:,:) :: rhidext0_grt -!> single scattering albedo +! single scattering albedo real (kind=kind_phys),allocatable, dimension(:,:) :: rhidssa0_grt -!> asymmetry parameter +! asymmetry parameter real (kind=kind_phys), allocatable, dimension(:,:) :: rhidasy0_grt ! ! relative humidity dependent aerosol optical properties: ! species : soot, suso, waso, ssam, sscm -!> \name relative humidity dependent aerosol optical properties: -!! species : soot, suso, waso, ssam, sscm +! \name relative humidity dependent aerosol optical properties: +! species : soot, suso, waso, ssam, sscm -!> extinction coefficient +! extinction coefficient real (kind=kind_phys),allocatable,dimension(:,:,:) :: rhdpext0_grt -!> single scattering albedo +! single scattering albedo real (kind=kind_phys),allocatable,dimension(:,:,:) :: rhdpssa0_grt -!> asymmetry parameter +! asymmetry parameter real (kind=kind_phys),allocatable,dimension(:,:,:) :: rhdpasy0_grt ! - relative humidity independent aerosol optical properties: @@ -467,31 +467,31 @@ module module_radiation_aerosols ! ! ssarhd_grt(KRHLEV,KCM2,NSWLWBD) - single scattering albedo for sw+lw band ! asyrhd_grt(KRHLEV,KCM2,NSWLWBD) - asymmetry parameter for sw+lw band -!>\name relative humidity independent aerosol optical properties +!\name relative humidity independent aerosol optical properties -!> extinction coefficient for SW+LW spectral band +! extinction coefficient for SW+LW spectral band real (kind=kind_phys),allocatable,save,dimension(:,:) :: & & extrhi_grt -!> single scattering albedo for SW+LW spectral band +! single scattering albedo for SW+LW spectral band real (kind=kind_phys),allocatable,save,dimension(:,:) :: & & ssarhi_grt -!> asymmetry parameter for SW+LW spectral band +! asymmetry parameter for SW+LW spectral band real (kind=kind_phys),allocatable,save,dimension(:,:) :: & & asyrhi_grt -!> \name relative humidity dependent aerosol optical properties +! \name relative humidity dependent aerosol optical properties -!> extinction coefficient for SW+LW spectral band +! extinction coefficient for SW+LW spectral band real (kind=kind_phys),allocatable,save,dimension(:,:,:) :: & & extrhd_grt -!> single scattering albedo for SW+LW band +! single scattering albedo for SW+LW band real (kind=kind_phys),allocatable,save,dimension(:,:,:) :: & & ssarhd_grt -!> asymmetry parameter for SW+LW band +! asymmetry parameter for SW+LW band real (kind=kind_phys),allocatable,save,dimension(:,:,:) :: & & asyrhd_grt -!> \name module variables for gocart aerosol clim data set +! \name module variables for gocart aerosol clim data set ! --------------------------------------------------------------------- ! ! section-5 : module variables for gocart aerosol climo data set ! @@ -509,14 +509,14 @@ module module_radiation_aerosols ! ! vertical coordinate (sigma for geos3/hybrid_sigma_pressure for geos4) ! aerosol units (mass concentration for geos3/mixing ratio for geos4) -!> num of lon-points in geos dataset +! num of lon-points in geos dataset integer, parameter :: IMXG = 144 -!> num of lat-points in geos dataset +! num of lat-points in geos dataset integer, parameter :: JMXG = 91 -!> num of vertical layers in geos dataset +! num of vertical layers in geos dataset integer, parameter :: KMXG = 30 !* integer, parameter :: NMXG = 12 -!> to be determined by set_aerspc +! to be determined by set_aerspc integer, save :: NMXG real (kind=kind_phys), parameter :: dltx = 360.0 / float(IMXG) @@ -528,22 +528,20 @@ module module_radiation_aerosols ! ! dmclmg - aerosol dry mass in g/m3 IMXG*JMXG*KMXG*NMXG ! or aerosol mixing ratio in mol/mol or Kg/Kg -!> pressure in cb +! pressure in cb real (kind=kind_phys),allocatable, save:: psclmg(:,:,:) -!> aerosol dry mass in g/m3 or aerosol mixing ration in mol/mol or Kg/Kg +! aerosol dry mass in g/m3 or aerosol mixing ration in mol/mol or Kg/Kg real (kind=kind_phys),allocatable, save:: dmclmg(:,:,:,:) ! - geos-gocart lat/lon arrays -!> geos-gocart longitude arrays real (kind=kind_phys), allocatable, save, dimension(:):: geos_rlon -!> geos-gocart latitude arrays real (kind=kind_phys), allocatable, save, dimension(:):: geos_rlat -!> control flag for gocart climo data set: xxxx as default; ver3 for geos3; +! control flag for gocart climo data set: xxxx as default; ver3 for geos3; !! ver4 for geos4; 0000 for unknown data character*4, save :: gocart_climo = 'xxxx' -!> molecular wght of gocart aerosol species +! molecular wght of gocart aerosol species real (kind=kind_io4), allocatable :: molwgt(:) ! --------------------------------------------------------------------- @@ -553,21 +551,21 @@ module module_radiation_aerosols ! ! --------------------------------------------------------------------- ! ! -!> logical parameter for gocart initialization control +! logical parameter for gocart initialization control logical, save :: lgrtint = .true. -!> logical parameter for gocart debug print control +! logical parameter for gocart debug print control ! logical, save :: lckprnt = .true. logical, save :: lckprnt = .false. ! --- the following index/flag/weight are set up in 'set_aerspc' -!> merging coefficients for fcst/clim; determined from fdaer +! merging coefficients for fcst/clim; determined from fdaer real (kind=kind_phys), save :: ctaer = f_zero ! user specified wgt -!> option to get fcst gocart aerosol field +! option to get fcst gocart aerosol field logical, save :: get_fcst = .true. -!> option to get clim gocart aerosol field +! option to get clim gocart aerosol field logical, save :: get_clim = .true. ! ------ gocart aerosol specification ------ @@ -588,8 +586,8 @@ module module_radiation_aerosols ! ! OC (waso) and BC (soot) ! -!> index for rh dependent aerosol optical properties (2nd -!! dimension for extrhd_grt, ssarhd_grt, and asyrhd_grt) +! index for rh dependent aerosol optical properties (2nd +! dimension for extrhd_grt, ssarhd_grt, and asyrhd_grt) integer, save :: isoot, iwaso, isuso, issam, isscm ! - index for rh independent aerosol optical properties (1st @@ -598,8 +596,6 @@ module module_radiation_aerosols ! ! - index for gocart aerosol species to be included in the ! calculations of aerosol optical properties (ext, ssa, asy) -!> index for gocart aerosol species to be included in the -!! calculations of aerosol optical properties (ext, ssa, asy) type gocart_index_type ! dust integer :: dust1, dust2, dust3, dust4, dust5 @@ -614,7 +610,7 @@ module module_radiation_aerosols ! endtype type (gocart_index_type), save :: dm_indx -!> index for gocart aerosols from prognostic tracer fields +! index for gocart aerosols from prognostic tracer fields type tracer_index_type ! dust integer :: du001, du002, du003, du004, du005 @@ -630,14 +626,14 @@ module module_radiation_aerosols ! type (tracer_index_type), save :: dmfcs_indx ! - grid components to be included in the aeropt calculations -!> number of aerosol grid components +! number of aerosol grid components integer, save :: num_gridcomp = 0 -!> aerosol grid components +! aerosol grid components character, allocatable , save :: gridcomp(:)*2 -!> default full-package setting +! default full-package setting integer, parameter :: max_num_gridcomp = 5 -!> data max_gridcomp /'DU', 'BC', 'OC', 'SU', 'SS'/ +! data max_gridcomp /'DU', 'BC', 'OC', 'SU', 'SS'/ character*2 :: max_gridcomp(max_num_gridcomp) data max_gridcomp /'DU', 'BC', 'OC', 'SU', 'SS'/ @@ -653,16 +649,16 @@ module module_radiation_aerosols ! ! idxspc (NCM) - index conversion array ! lspcaod - logical flag for aod from individual species ! -!> index conversion array:data idxspc / 1, 2, 1, 1, 1, 1, 3, 5, 5, 4 / +! index conversion array:data idxspc / 1, 2, 1, 1, 1, 1, 3, 5, 5, 4 / integer, dimension(NCM) :: idxspc data idxspc / 1, 2, 1, 1, 1, 1, 3, 5, 5, 4 / ! ! - wvn550 is the wavenumber (1/cm) of wavelenth 550nm for diagnostic aod output ! nv_aod is the sw spectral band covering wvn550 (comp in aer_init) ! -!> the wavenumber (\f$cm^-1\f$) of wavelength 550nm for diagnostic aod output +! the wavenumber (\f$cm^-1\f$) of wavelength 550nm for diagnostic aod output real (kind=kind_phys), parameter :: wvn550 = 1.0e4/0.55 -!> the sw spectral band covering wvn550 (comp in aer_init) +! the sw spectral band covering wvn550 (comp in aer_init) integer, save :: nv_aod = 1 ! --- public interfaces diff --git a/physics/radiation_astronomy.f b/physics/radiation_astronomy.f index adfc028f1..1fe155ea2 100644 --- a/physics/radiation_astronomy.f +++ b/physics/radiation_astronomy.f @@ -108,28 +108,28 @@ module module_radiation_astronomy ! ! real (kind=kind_phys), parameter :: pid12 = con_pi/f12 ! angle per hour real (kind=kind_phys), parameter :: pid12 = (2.0*asin(1.0))/f12 -!> \name Module variable (to be set in module_radiation_astronomy::sol_init): +! \name Module variable (to be set in module_radiation_astronomy::sol_init): real (kind=kind_phys), public :: solc0 = con_solr integer :: isolflg = 10 character(26) :: solar_fname = ' ' -!> \name Module variables (to be set in module_radiation_astronomy::sol_update) +! \name Module variables (to be set in module_radiation_astronomy::sol_update) -!> equation of time +! equation of time real (kind=kind_phys) :: sollag=0.0 -!> sine of the solar declination angle +! sine of the solar declination angle real (kind=kind_phys) :: sindec=0.0 -!> cosine of the solar declination angle +! cosine of the solar declination angle real (kind=kind_phys) :: cosdec=0.0 -!> solar angle increment per interation of cosz calc +! solar angle increment per interation of cosz calc real (kind=kind_phys) :: anginc=0.0 -!> saved monthly solar constants (isolflg=4 only) +! saved monthly solar constants (isolflg=4 only) real (kind=kind_phys) :: smon_sav(12) data smon_sav(1:12) / 12*con_solr / -!> saved year of data used +! saved year of data used integer :: iyr_sav =0 -!> total number of zenith angle iterations +! total number of zenith angle iterations integer :: nstp =6 public sol_init, sol_update, coszmn diff --git a/physics/radiation_clouds.f b/physics/radiation_clouds.f index 1164c4e31..654e320ad 100644 --- a/physics/radiation_clouds.f +++ b/physics/radiation_clouds.f @@ -160,16 +160,17 @@ !! the fraction of clouds; (iii) effective radius of water/ice droplet: !!\version NCEP-Radiation_clouds v5.1 Nov 2012 !! -!! This module has three externally accessible subroutines: -!! - cld_init() --- initialization routine -!! - progcld1() --- zhao/moorthi prognostic cloud scheme -!! - progcld2() --- ferrier prognostic cloud microphysics -!! - progcld3() --- zhao/moorthi prognostic cloud + pdfcld -!! - diagcld1() --- diagnostic cloud calculation routine +!! This module has six externally accessible subroutines: +!! - cld_init():initialization routine +!! - progcld1():zhao/moorthi prognostic cloud scheme +!! - progcld2():Ferrier prognostic cloud microphysics +!! - progcld3():Zhao/Moorthi prognostic cloud + pdfcld +!! - progclduni():unified clouds with MG microphys +!! - diagcld1():diagnostic cloud calculation routine !! !! and two internally accessable only subroutines: -!! - gethml() --- get diagnostic hi, mid, low,total,BL clouds -!! - rhtable() --- rh lookup table for diag cloud scheme +!! - gethml():get diagnostic hi, mid, low,total,BL clouds +!! - rhtable():rh lookup table for diag cloud scheme !! !> \section gen_al General Algorithm !! @{ @@ -253,12 +254,12 @@ module module_radiation_clouds ! ! --- set constant parameters real (kind=kind_phys), parameter :: gfac=1.0e5/con_g & &, gord=con_g/con_rd -!> number of fields in cloud array +! number of fields in cloud array integer, parameter, public :: NF_CLDS = 9 -!> number of cloud vertical domains +! number of cloud vertical domains integer, parameter, public :: NK_CLDS = 3 -!> pressure limits of cloud domain interfaces (low,mid,high) in mb (0.1kPa) +! pressure limits of cloud domain interfaces (low,mid,high) in mb (0.1kPa) real (kind=kind_phys), save :: ptopc(NK_CLDS+1,2) !org data ptopc / 1050., 642., 350., 0.0, 1050., 750., 500., 0.0 / @@ -268,56 +269,56 @@ module module_radiation_clouds ! real (kind=kind_phys), parameter :: climit = 0.001, climit2=0.05 real (kind=kind_phys), parameter :: ovcst = 1.0 - 1.0e-8 -!> default liq radius to 10 micron +! default liq radius to 10 micron real (kind=kind_phys), parameter :: reliq_def = 10.0 -!> default ice radius to 50 micron +! default ice radius to 50 micron real (kind=kind_phys), parameter :: reice_def = 50.0 -!> default rain radius to 1000 micron +! default rain radius to 1000 micron real (kind=kind_phys), parameter :: rrain_def = 1000.0 -!> default snow radius to 250 micron +! default snow radius to 250 micron real (kind=kind_phys), parameter :: rsnow_def = 250.0 -!> rh in one percent interval +! rh in one percent interval integer, parameter :: NBIN=100 -!> =1,2 for eastern and western hemispheres +! =1,2 for eastern and western hemispheres integer, parameter :: NLON=2 -!> =1,4 for 60n-30n,30n-equ,equ-30s,30s-60s +! =1,4 for 60n-30n,30n-equ,equ-30s,30s-60s integer, parameter :: NLAT=4 -!> =1,4 for bl,low,mid,hi cld type +! =1,4 for bl,low,mid,hi cld type integer, parameter :: MCLD=4 -!> =1,2 for land,sea +! =1,2 for land,sea integer, parameter :: NSEAL=2 -!> default cld single scat albedo +! default cld single scat albedo real (kind=kind_phys), parameter :: cldssa_def = 0.99 -!> default cld asymmetry factor +! default cld asymmetry factor real (kind=kind_phys), parameter :: cldasy_def = 0.84 ! --- xlabdy: lat bndry between tuning regions, +/- xlim for transition ! xlobdy: lon bndry between tuning regions -!> lat bndry between tuning regions +! lat bndry between tuning regions real (kind=kind_phys) :: xlabdy(3) -!> lon bndry between tuning regions +! lon bndry between tuning regions real (kind=kind_phys) :: xlobdy(3) -!> +/- xlim for transition +! +/- xlim for transition real (kind=kind_phys), parameter :: xlim=5.0 data xlabdy / 30.0, 0.0, -30.0 /, xlobdy / 0.0, 180., 360. / -!> low cloud vertical velocity adjustment boundaries in mb/sec +! low cloud vertical velocity adjustment boundaries in mb/sec real (kind=kind_phys), parameter :: vvcld1= 0.0003e0 -!> low cloud vertical velocity adjustment boundaries in mb/sec +! low cloud vertical velocity adjustment boundaries in mb/sec real (kind=kind_phys), parameter :: vvcld2=-0.0005e0 ! --- those data will be set up by "cld_init" ! rhcl : tuned rh relation table for diagnostic cloud scheme -!> tuned relative humidity relation table for diagnostic cloud scheme +! tuned relative humidity relation table for diagnostic cloud scheme real (kind=kind_phys) :: rhcl(NBIN,NLON,NLAT,MCLD,NSEAL) -!> upper limit of boundary layer clouds +! upper limit of boundary layer clouds integer :: llyr = 2 -!> maximum-random cloud overlapping method +! maximum-random cloud overlapping method integer :: iovr = 1 public progcld1, progcld2, progcld3, progclduni, diagcld1, & diff --git a/physics/radiation_gases.f b/physics/radiation_gases.f index 0cac550f5..75b57fcf8 100644 --- a/physics/radiation_gases.f +++ b/physics/radiation_gases.f @@ -136,42 +136,42 @@ module module_radiation_gases ! & VTAGGAS='NCEP-Radiation_gases v5.1 Nov 2012 ' ! & VTAGGAS='NCEP-Radiation_gases v5.0 Aug 2012 ' -!>\name parameter constants +! \name parameter constants -!> number of gas species +! number of gas species integer, parameter, public :: NF_VGAS = 10 -!> input co2 dat lon points +! input co2 dat lon points integer, parameter :: IMXCO2 = 24 -!> input co2 data lat points +! input co2 data lat points integer, parameter :: JMXCO2 = 12 -!> earlist year 2-d co2 data available +! earlist year 2-d co2 data available integer, parameter :: MINYEAR = 1957 -!> horizontal resolution in degree +! horizontal resolution in degree real (kind=kind_phys), parameter :: resco2=15.0 -!> rad->deg conversion +! rad->deg conversion real (kind=kind_phys), parameter :: raddeg=180.0/con_pi -!> pressure limitation for 2-d co2 (mb) +! pressure limitation for 2-d co2 (mb) real (kind=kind_phys), parameter :: prsco2=788.0 -!> half of pi +! half of pi real (kind=kind_phys), parameter :: hfpi =0.5*con_pi -!>\name parameter constants for gas volume mixing ratioes +!\name parameter constants for gas volume mixing ratioes real (kind=kind_phys), parameter :: co2vmr_def = 350.0e-6 real (kind=kind_phys), parameter :: n2ovmr_def = 0.31e-6 real (kind=kind_phys), parameter :: ch4vmr_def = 1.50e-6 real (kind=kind_phys), parameter :: o2vmr_def = 0.209 real (kind=kind_phys), parameter :: covmr_def = 1.50e-8 -!> aer 2003 value +! aer 2003 value real (kind=kind_phys), parameter :: f11vmr_def = 3.520e-10 -!> aer 2003 value +! aer 2003 value real (kind=kind_phys), parameter :: f12vmr_def = 6.358e-10 -!> aer 2003 value +! aer 2003 value real (kind=kind_phys), parameter :: f22vmr_def = 1.500e-10 -!> aer 2003 value +! aer 2003 value real (kind=kind_phys), parameter :: cl4vmr_def = 1.397e-10 -!> gfdl 1999 value +! gfdl 1999 value real (kind=kind_phys), parameter :: f113vmr_def= 8.2000e-11 ! --- ozone seasonal climatology parameters defined in module ozne_def @@ -184,13 +184,13 @@ module module_radiation_gases ! ! --- module variables to be set in subroutin gas_init and/or gas_update -!> \name variables for climatology ozone (ioznflg = 0) +! \name variables for climatology ozone (ioznflg = 0) real (kind=kind_phys), allocatable :: pkstr(:), o3r(:,:,:) integer :: k1oz = 0, k2oz = 0 real (kind=kind_phys) :: facoz = 0.0 -!>\name arrays for co2 2-d monthly data and global mean values from observed data +!\name arrays for co2 2-d monthly data and global mean values from observed data real (kind=kind_phys), allocatable :: co2vmr_sav(:,:,:) real (kind=kind_phys), allocatable :: co2cyc_sav(:,:,:) diff --git a/physics/radiation_surface.f b/physics/radiation_surface.f index d2ca4e79e..9b5107906 100644 --- a/physics/radiation_surface.f +++ b/physics/radiation_surface.f @@ -99,22 +99,22 @@ module module_radiation_surface ! ! & VTAGSFC='NCEP-Radiation_surface v5.0 Aug 2012 ' ! --- constant parameters -!> num of sfc albedo components +! num of sfc albedo components integer, parameter, public :: NF_ALBD = 4 -!> num of longitude points in global emis-type map +! num of longitude points in global emis-type map integer, parameter, public :: IMXEMS = 360 -!> num of latitude points in global emis-type map +! num of latitude points in global emis-type map integer, parameter, public :: JMXEMS = 180 real (kind=kind_phys), parameter :: f_zero = 0.0 real (kind=kind_phys), parameter :: f_one = 1.0 real (kind=kind_phys), parameter :: rad2dg= 180.0 / con_pi -!> global surface emissivity index array +! global surface emissivity index array integer, allocatable :: idxems(:,:) -!> global surface emissivity contrl flag set up in 'sfc_init' +! global surface emissivity contrl flag set up in 'sfc_init' integer :: iemslw = 0 ! public sfc_init, setalb, setemis diff --git a/physics/radlw_datatb.f b/physics/radlw_datatb.f index 6918da230..30b9bd376 100644 --- a/physics/radlw_datatb.f +++ b/physics/radlw_datatb.f @@ -5,6 +5,8 @@ !! - module_radlw_cldprlw (cloud property coefficients) !! - module_radlw_kgbnn (absorption coeffients for 16 bands, !! where nn = 01-16) +!> \defgroup radlw_datatb GFS RADLW datatb Modules +!!\ingroup RRTMG ! ============================================================== !!!!! ! lw-rrtm3 radiation package description !!!!! @@ -61,7 +63,7 @@ !!!!! end descriptions !!!!! !!!!! ============================================================== !!!!! -!> \ingroup module_radlw_main +!> \ingroup radlw_datatb !> This module contains plank flux data. !========================================! module module_radlw_avplank ! @@ -738,7 +740,7 @@ module module_radlw_avplank ! end module module_radlw_avplank ! !========================================! -!> \ingroup module_radlw_main +!> \ingroup radlw_datatb !> This module contains reference temperature and pressure. !! !! - These pressures are chosen such that the ln of the first one @@ -922,7 +924,7 @@ module module_radlw_ref ! end module module_radlw_ref ! !========================================! -!> \ingroup module_radlw_main +!> \ingroup radlw_datatb !> This module contains cloud property coefficients. !========================================! module module_radlw_cldprlw ! @@ -1583,8 +1585,7 @@ module module_radlw_cldprlw ! end module module_radlw_cldprlw ! !========================================! -!> \defgroup module_radlw_kgbnn module_radlw_kgbnn -!! \ingroup module_radlw_main +!> \ingroup radlw_datatb !! @{ !*********************************************************************! @@ -1608,6 +1609,7 @@ end module module_radlw_cldprlw ! ! ! ! ********* ********* end description ********* ********* ! +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 01: 10-250 !! cm-1 (low - h2o; high - h2o) !========================================! @@ -2422,6 +2424,7 @@ module module_radlw_kgb01 ! end module module_radlw_kgb01 ! !========================================! +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 02: 250-500 !! cm-1 (low - h2o; high - h2o) !========================================! @@ -3279,7 +3282,7 @@ module module_radlw_kgb02 ! end module module_radlw_kgb02 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 03: 500-630 !! cm-1 (low - h2o, co2; high - h2o, co2) !========================================! @@ -10154,7 +10157,7 @@ module module_radlw_kgb03 ! end module module_radlw_kgb03 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 04: 630-700 !! cm-1 (low - h2o, co2; high - co2, o3) !========================================! @@ -15355,7 +15358,7 @@ module module_radlw_kgb04 ! end module module_radlw_kgb04 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 05: 700-820 !! cm-1 (low - h2o, co2; high - co2, o3) !========================================! @@ -21853,7 +21856,7 @@ module module_radlw_kgb05 ! end module module_radlw_kgb05 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 06: 820-980 !! cm-1 (low - h2o; high - /) !========================================! @@ -22114,7 +22117,7 @@ module module_radlw_kgb06 ! end module module_radlw_kgb06 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 07: 980-1080 !! cm-1 (low - h2o, o3; high - o3) !========================================! @@ -24762,7 +24765,7 @@ module module_radlw_kgb07 ! end module module_radlw_kgb07 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 08: 1080-1180 !! cm-1 (low - h2o; high - o3) !========================================! @@ -25560,6 +25563,7 @@ module module_radlw_kgb08 ! end module module_radlw_kgb08 ! !========================================! +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 09: 1180-1390 !! cm-1 (low - h2o, ch4; high - ch4) !========================================! @@ -28238,7 +28242,7 @@ module module_radlw_kgb09 ! end module module_radlw_kgb09 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 10: 1390-1480 !! cm-1 (low - h2o; high - h2o) !========================================! @@ -28713,7 +28717,7 @@ module module_radlw_kgb10 ! end module module_radlw_kgb10 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 11: 1480-1800 !! cm-1 (low - h2o; high - h2o) !========================================! @@ -29413,7 +29417,7 @@ module module_radlw_kgb11 ! end module module_radlw_kgb11 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 12: 1800-2080 !! cm-1 (low - h2o, co2; high - /) !========================================! @@ -30485,7 +30489,7 @@ module module_radlw_kgb12 ! end module module_radlw_kgb12 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 13: 2080-2250 !! cm-1 (low - h2o, n2o; high - /) !========================================! @@ -31392,7 +31396,7 @@ module module_radlw_kgb13 ! end module module_radlw_kgb13 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 14: 2250-2380 !! cm-1 (low - co2; high - co2) !========================================! @@ -31617,7 +31621,7 @@ module module_radlw_kgb14 ! end module module_radlw_kgb14 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 15: 2380-2600 !! cm-1 (low - n2o, co2; high - /) !========================================! @@ -32023,7 +32027,7 @@ module module_radlw_kgb15 ! end module module_radlw_kgb15 ! !========================================! - +!> \ingroup radlw_datatb !> This module sets up absorption coefficients for band 16: 2600-3000 !! cm-1 (low - h2o, ch4; high - /) !========================================! diff --git a/physics/radlw_main.f b/physics/radlw_main.f index 04abd2c1f..466f5ca1e 100644 --- a/physics/radlw_main.f +++ b/physics/radlw_main.f @@ -326,7 +326,7 @@ !> \defgroup module_radlw_main GFS RADLW Main !! \ingroup RRTMG -!! This module includes NCEP's modifications of the rrtmg-lw radiation +!! This module includes NCEP's modifications of the RRTMG-LW radiation !! code from AER. !! !! The RRTM-LW package includes three files: @@ -338,14 +338,8 @@ !! - module_radlw_cldprlw: cloud property coefficients !! - module_radlw_kgbnn: absorption coeffients for 16 bands, where nn = 01-16 !! - radlw_main.f, which contains: -!! - module_radlw_main, which is the main LW radiation transfer -!! program and contains two externally callable subroutines: -!! - lwrad_run(): the main LW radiation routine -!! - rlwinit(): the initialization routine -!! -!! All the LW radiation subprograms become contained subprograms in -!! module 'module_radlw_main' and many of them are not directly -!! accessable from places outside the module. +!! - lwrad_run(): the main LW radiation routine +!! - rlwinit(): the initialization routine !! !!\author Eli J. Mlawer, emlawer@aer.com !!\author Jennifer S. Delamere, jdelamer@aer.com @@ -481,6 +475,7 @@ module module_radlw_main ! subroutine lwrad_init () end subroutine lwrad_init +!>\ingroup module_radlw_main !> This subroutine is the main LW radiation routine. !! \section arg_table_lwrad_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -1347,6 +1342,7 @@ subroutine lwrad_finalize () end subroutine lwrad_finalize +!>\ingroup module_radlw_main !> This subroutine performs calculations necessary for the initialization !! of the longwave model. lookup tables are computed for use in the lw !! radiative transfer, and input absorption coefficient data for each @@ -3949,8 +3945,8 @@ subroutine taumol & contains ! ================= -!> band 1: 10-350 cm-1 (low key - h2o; low minor - n2); -!! (high key - h2o; high minor - n2) +! band 1: 10-350 cm-1 (low key - h2o; low minor - n2); +! (high key - h2o; high minor - n2) ! ---------------------------------- subroutine taugb01 ! .................................. diff --git a/physics/radlw_param.f b/physics/radlw_param.f index c7a79c68a..07d081271 100644 --- a/physics/radlw_param.f +++ b/physics/radlw_param.f @@ -1,7 +1,8 @@ !> \file radlw_param.f !! This file contains LW band parameters setup. -!> \ingroup module_radlw_main +!> \defgroup radlw_param GFS RADLW param Module +!!\ingroup RRTMG !! @{ !!!!! ============================================================== !!!!! @@ -59,6 +60,7 @@ !!!!! end descriptions !!!!! !!!!! ============================================================== !!!!! +!>\ingroup radlw_param !> This module contains LW band parameters set up. !========================================! module module_radlw_parameters ! @@ -71,79 +73,79 @@ module module_radlw_parameters ! public ! ! -!> Define type construct for radiation fluxes at toa. +! Define type construct for radiation fluxes at toa. type :: topflw_type -!> total sky upward flux at toa +! total sky upward flux at toa real (kind=kind_phys) :: upfxc -!> clear sky upward flux at toa +! clear sky upward flux at toa real (kind=kind_phys) :: upfx0 end type ! ! -!> Define type construct for radiation fluxes at surface. +! Define type construct for radiation fluxes at surface. type :: sfcflw_type -!> total sky upward flux at sfc +! total sky upward flux at sfc real (kind=kind_phys) :: upfxc -!> clear sky upward flux at sfc +! clear sky upward flux at sfc real (kind=kind_phys) :: upfx0 -!> total sky downward flux at sfc +! total sky downward flux at sfc real (kind=kind_phys) :: dnfxc -!> clear sky downward flux at sfc +! clear sky downward flux at sfc real (kind=kind_phys) :: dnfx0 end type ! ! -!> Define type construct for optional radiation flux profiles. +! Define type construct for optional radiation flux profiles. type :: proflw_type -!> level up flux for total sky +! level up flux for total sky real (kind=kind_phys) :: upfxc -!> level dn flux for total sky +! level dn flux for total sky real (kind=kind_phys) :: dnfxc -!> level up flux fro clear sky +! level up flux fro clear sky real (kind=kind_phys) :: upfx0 -!> level dn flux for clear sky +! level dn flux for clear sky real (kind=kind_phys) :: dnfx0 end type ! -!>\name Parameter constants for LW band structures +!\name Parameter constants for LW band structures -!> num of total spectral bands +! num of total spectral bands integer, parameter :: NBANDS = 16 -!> num of total g-points +! num of total g-points integer, parameter :: NGPTLW = 140 -!> lookup table dimension +! lookup table dimension integer, parameter :: NTBL = 10000 -!> max num of absorbing gases +! max num of absorbing gases integer, parameter :: MAXGAS = 7 -!> num of halocarbon gasees +! num of halocarbon gasees integer, parameter :: MAXXSEC= 4 -!> num of ref rates of binary species +! num of ref rates of binary species integer, parameter :: NRATES = 6 -!> dim for plank function table +! dim for plank function table integer, parameter :: NPLNK = 181 integer, parameter :: NBDLW = NBANDS -!> \name Number of g-point in each band +! \name Number of g-point in each band integer :: NG01, NG02, NG03, NG04, NG05, NG06, NG07, NG08, & NG09, NG10, NG11, NG12, NG13, NG14, NG15, NG16 parameter (NG01=10, NG02=12, NG03=16, NG04=14, NG05=16, NG06=08, & NG07=12, NG08=08, NG09=12, NG10=06, NG11=08, NG12=08, & NG13=04, NG14=02, NG15=02, NG16=02) -!> \name Begining index of each band +! \name Begining index of each band integer :: NS01, NS02, NS03, NS04, NS05, NS06, NS07, NS08, & NS09, NS10, NS11, NS12, NS13, NS14, NS15, NS16 parameter (NS01=00, NS02=10, NS03=22, NS04=38, NS05=52, NS06=68, & NS07=76, NS08=88, NS09=96, NS10=108, NS11=114, & NS12=122, NS13=130, NS14=134, NS15=136, NS16=138) -!> band indices for each g-point +! band indices for each g-point integer, dimension(NGPTLW) :: NGB data NGB(:) / 10*1, 12*2, 16*3, 14*4, 16*5, 8*6, 12*7, 8*8, & ! band 1- 8 & 12*9, 6*10, 8*11, 8*12, 4*13, 2*14, 2*15, 2*16 / ! band 9-16 -!> \name Band spectrum structures (wavenumber is 1/cm +! \name Band spectrum structures (wavenumber is 1/cm real (kind=kind_phys) :: wvnlw1(NBANDS), wvnlw2(NBANDS) data wvnlw1 / & & 10., 351., 501., 631., 701., 821., 981., 1081., & diff --git a/physics/radsw_datatb.f b/physics/radsw_datatb.f index 4df54db8b..38034ca2e 100644 --- a/physics/radsw_datatb.f +++ b/physics/radsw_datatb.f @@ -6,6 +6,8 @@ !! - module_radsw_sflux (spectral solar flux distribution) !! - module_radsw_kgbnn (absorption coeffients for 14 bands, !! where nn = 16-29) +!>\defgroup radsw_datatb GFS RADSW datatb Modules +!!\ingroup RRTMG ! ============================================================== !!!!! ! sw-rrtm3 radiation package description !!!!! @@ -63,7 +65,7 @@ !!!!! ============================================================== !!!!! -!> \ingroup module_radsw_main +!> \ingroup radsw_datatb !> This module contains the reference pressures (in logarithm form) at !! 59 vertical levels (TOA is omitted), and the mid-latitude summer !! (MLS) standard temperature profile for the 59 pressure layers that @@ -136,7 +138,7 @@ module module_radsw_ref ! end module module_radsw_ref ! !========================================! -!> \ingroup module_radsw_main +!> \ingroup radsw_datatb !> This module contains cloud radiative property coefficients. !! !! For liquid water clouds, cloud radiative property coefficients are @@ -1924,7 +1926,7 @@ module module_radsw_cldprtb ! end module module_radsw_cldprtb ! !========================================! -!> \ingroup module_radsw_main +!> \ingroup radsw_datatb !> This module contains various indexes and coefficients for SW spectral !! bands, as well as the spectral distribution of solar flux. The values !! of spectral solar flux are derived based on a prescribed solar @@ -2264,10 +2266,7 @@ module module_radsw_sflux ! end module module_radsw_sflux ! !========================================! -!>\defgroup module_radsw_kgbnn module_radsw_kgbnn -!>\ingroup module_radsw_main -!! @{ - +!>\ingroup radsw_datatb !> This module sets up absorption coefficients for band 16: 2600-3250 !! cm-1 (low - h2o, ch4; high - ch4) !========================================! @@ -3461,7 +3460,7 @@ module module_radsw_kgb16 ! end module module_radsw_kgb16 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 17: 3250-4000 !! cm-1 (low - h2o,co2; high - h2o,co2) !========================================! @@ -8071,7 +8070,7 @@ module module_radsw_kgb17 ! end module module_radsw_kgb17 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 18: 4000-4650 !! cm-1 (low - h2o,ch4; high - ch4) !========================================! @@ -9590,6 +9589,7 @@ module module_radsw_kgb18 ! end module module_radsw_kgb18 ! !========================================! +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 19: 4650-5150 !! cm-1 (low - h2o,co2; high - co2) !========================================! @@ -11109,7 +11109,7 @@ module module_radsw_kgb19 ! end module module_radsw_kgb19 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 20: 5150-6150 !! cm-1 (low - h2o; high - h2o) !========================================! @@ -11894,7 +11894,7 @@ module module_radsw_kgb20 ! end module module_radsw_kgb20 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 21: 6150-7700 !! cm-1 (low - h2o,co2; high - h2o,co2) !========================================! @@ -15753,6 +15753,7 @@ module module_radsw_kgb21 ! end module module_radsw_kgb21 ! !========================================! +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 22: 7700-8050 !! cm-1 (low - h2o, o2; high - o2) !========================================! @@ -16200,7 +16201,7 @@ module module_radsw_kgb22 ! end module module_radsw_kgb22 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 23: 8050-12850 !! cm-1 (low - h2o; high - nothing) !========================================! @@ -16458,6 +16459,7 @@ module module_radsw_kgb23 ! end module module_radsw_kgb23 ! !========================================! +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 24: 12850-16000 !! cm-1 (low - h2o, o2; high - o2) !========================================! @@ -18023,7 +18025,7 @@ module module_radsw_kgb24 ! end module module_radsw_kgb24 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 25: 16000-22650 !! cm-1 (low - h2o; high - nothing) !========================================! @@ -18184,7 +18186,7 @@ module module_radsw_kgb25 ! end module module_radsw_kgb25 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 26: 22650-29000 !! cm-1 (low - nothing; high - nothing) !========================================! @@ -18221,7 +18223,7 @@ module module_radsw_kgb26 ! end module module_radsw_kgb26 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 27: 29000-38000 !! cm-1 (low - o3; high - o3) !========================================! @@ -18825,7 +18827,7 @@ module module_radsw_kgb27 ! end module module_radsw_kgb27 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 28: 38000-50000 !! cm-1 (low - o3,o2; high - o3,o2) !========================================! @@ -21140,7 +21142,7 @@ module module_radsw_kgb28 ! end module module_radsw_kgb28 ! !========================================! - +!>\ingroup radsw_datatb !> This module sets up absorption coeffients for band 29: 820-2600 !! cm-1 (low - h2o; high - co2) !========================================! @@ -22081,4 +22083,3 @@ module module_radsw_kgb29 ! !........................................! end module module_radsw_kgb29 ! !========================================! -!! @} diff --git a/physics/radsw_main.f b/physics/radsw_main.f index 253494d42..af512d47a 100644 --- a/physics/radsw_main.f +++ b/physics/radsw_main.f @@ -262,7 +262,7 @@ !> \ingroup RRTMG !! \defgroup module_radsw_main GFS RADSW Main -!! This module includes NCEP's modifications of the rrtmg-sw radiation +!! This module includes NCEP's modifications of the RRTMG-SW radiation !! code from AER. !! !! The SW radiation model in the current NOAA Environmental Modeling @@ -381,10 +381,8 @@ !! - mersenne_twister: program of random number generators using the !! Mersenne-Twister algorithm !! - radsw_main.f, which contains: -!! - module_radsw_main: the main SW radiation computation programming -!! source codes, which contains two externally callable subroutines: -!! - swrad(): the main radiation routine -!! - rswinit(): the initialization routine +!! - swrad_run(): the main radiation routine +!! - rswinit(): the initialization routine !! !!\author Eli J. Mlawer, emlawer@aer.com !!\author Jennifer S. Delamere, jdelamer@aer.com @@ -434,30 +432,30 @@ module module_radsw_main ! ! & VTAGSW='RRTM-SW 112v2.3 Mar 2005' ! & VTAGSW='RRTM-SW 112v2.0 Jul 2004' -!> \name constant values +! \name constant values real (kind=kind_phys), parameter :: eps = 1.0e-6 real (kind=kind_phys), parameter :: oneminus= 1.0 - eps -!> pade approx constant +! pade approx constant real (kind=kind_phys), parameter :: bpade = 1.0/0.278 real (kind=kind_phys), parameter :: stpfac = 296.0/1013.0 real (kind=kind_phys), parameter :: ftiny = 1.0e-12 real (kind=kind_phys), parameter :: flimit = 1.0e-20 -!> internal solar constant +! internal solar constant real (kind=kind_phys), parameter :: s0 = 1368.22 real (kind=kind_phys), parameter :: f_zero = 0.0 real (kind=kind_phys), parameter :: f_one = 1.0 -!> \name atomic weights for conversion from mass to volume mixing ratios +! \name atomic weights for conversion from mass to volume mixing ratios real (kind=kind_phys), parameter :: amdw = con_amd/con_amw real (kind=kind_phys), parameter :: amdo3 = con_amd/con_amo3 -!> \name band indices +! \name band indices integer, dimension(nblow:nbhgh) :: nspa, nspb -!> band index for sfc flux +! band index for sfc flux integer, dimension(nblow:nbhgh) :: idxsfc -!> band index for cld prop +! band index for cld prop integer, dimension(nblow:nbhgh) :: idxebc data nspa(:) / 9, 9, 9, 9, 1, 9, 9, 1, 9, 1, 0, 1, 9, 1 / @@ -480,26 +478,26 @@ module module_radsw_main ! ! & 650.0, 750.0, 650.0, 500.0, 1000.0, 1550.0, 350.0, & ! & 4800.0, 3150.0, 6650.0, 6350.0, 9000.0,12000.0, 1780.0 / -!> uv-b band index +! uv-b band index integer, parameter :: nuvb = 27 -!>\name logical flags for optional output fields +!\name logical flags for optional output fields logical :: lhswb = .false. logical :: lhsw0 = .false. logical :: lflxprf= .false. logical :: lfdncmp= .false. -!> those data will be set up only once by "rswinit" +! those data will be set up only once by "rswinit" real (kind=kind_phys) :: exp_tbl(0:NTBMX) -!> the factor for heating rates (in k/day, or k/sec set by subroutine +! the factor for heating rates (in k/day, or k/sec set by subroutine !! 'rswinit') real (kind=kind_phys) :: heatfac -!> initial permutation seed used for sub-column cloud scheme +! initial permutation seed used for sub-column cloud scheme integer, parameter :: ipsdsw0 = 1 ! --- public accessable subprograms @@ -515,6 +513,7 @@ module module_radsw_main ! subroutine swrad_init () end subroutine swrad_init +!>\ingroup module_radsw_main !>/brief This subroutine is the main SW radiation routine. !! \section arg_table_swrad_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -1397,6 +1396,7 @@ subroutine swrad_finalize () end subroutine swrad_finalize +!>\ingroup module_radsw_main !> This subroutine initializes non-varying module variables, conversion !! factors, and look-up tables. !!\param me print control for parallel process @@ -4178,7 +4178,7 @@ subroutine taumol & contains ! ================= -!> The subroutine computes the optical depth in band 16: 2600-3250 +! The subroutine computes the optical depth in band 16: 2600-3250 !! cm-1 (low - h2o,ch4; high - ch4) !----------------------------------- subroutine taumol16 diff --git a/physics/radsw_param.f b/physics/radsw_param.f index f2588cb18..d646fbf5e 100644 --- a/physics/radsw_param.f +++ b/physics/radsw_param.f @@ -1,7 +1,8 @@ !> \file radsw_param.f !! This file contains SW band parameters setup. -!> \ingroup module_radsw_main +!> \defgroup radsw_param GFS RADSW param Module +!! \ingroup RRTMG !! @{ !!!!! ============================================================== !!!!! @@ -59,7 +60,7 @@ !!!!! end descriptions !!!!! !!!!! ============================================================== !!!!! - +!>\ingroup radsw_param !> This module is for specifying the band structures and program parameters !! used by the RRTMG-SW scheme. !========================================! @@ -72,79 +73,79 @@ module module_radsw_parameters ! ! public ! -!> derived type for SW fluxes at TOA +! derived type for SW fluxes at TOA type :: topfsw_type -!> total-sky upward flux +! total-sky upward flux real (kind=kind_phys) :: upfxc -!> total-sky downward flux +! total-sky downward flux real (kind=kind_phys) :: dnfxc -!> clear-sky upward flux +! clear-sky upward flux real (kind=kind_phys) :: upfx0 end type ! -!> derived type for SW fluxes at surface +! derived type for SW fluxes at surface type :: sfcfsw_type -!> total-sky upward flux +! total-sky upward flux real (kind=kind_phys) :: upfxc -!> total-sky downward flux +! total-sky downward flux real (kind=kind_phys) :: dnfxc -!> clear-sky upward flux +! clear-sky upward flux real (kind=kind_phys) :: upfx0 -!> clear-sky downward flux +! clear-sky downward flux real (kind=kind_phys) :: dnfx0 end type ! -!> derived type for SW fluxes' column profiles (at layer interfaces) +! derived type for SW fluxes' column profiles (at layer interfaces) type :: profsw_type -!> total-sky upward flux +! total-sky upward flux real (kind=kind_phys) :: upfxc -!> total-sky downward flux +! total-sky downward flux real (kind=kind_phys) :: dnfxc -!> clear-sky upward flux +! clear-sky upward flux real (kind=kind_phys) :: upfx0 -!> clear-sky downward flux +! clear-sky downward flux real (kind=kind_phys) :: dnfx0 end type ! -!> derived type for special components of surface SW fluxes +! derived type for special components of surface SW fluxes type :: cmpfsw_type -!> total-sky downward flux cover UV-B spectrum +! total-sky downward flux cover UV-B spectrum real (kind=kind_phys) :: uvbfc -!> clear-sky downward flux cover UV-B spectrum +! clear-sky downward flux cover UV-B spectrum real (kind=kind_phys) :: uvbf0 -!> total-sky downward flux for near-IR direct beam +! total-sky downward flux for near-IR direct beam real (kind=kind_phys) :: nirbm -!> total-sky downward flux for near-IR diffused part +! total-sky downward flux for near-IR diffused part real (kind=kind_phys) :: nirdf -!> total-sky downward flux for UV+Visible direct +! total-sky downward flux for UV+Visible direct real (kind=kind_phys) :: visbm -!> total-sky downward flux for UV+Visible diffused +! total-sky downward flux for UV+Visible diffused real (kind=kind_phys) :: visdf end type ! -!! \name Parameter constants for SW band structures +! \name Parameter constants for SW band structures -!> band range lower index +! band range lower index integer, parameter :: NBLOW = 16 -!> band range upper index +! band range upper index integer, parameter :: NBHGH = 29 -!> total number of SW bands (14) +! total number of SW bands (14) integer, parameter :: NBANDS = NBHGH-NBLOW+1 -!> total number of g-point in all bands +! total number of g-point in all bands integer, parameter :: NGPTSW = 112 -!> maximum number of g-point in one band +! maximum number of g-point in one band integer, parameter :: NGMAX = 16 -!> maximum number of absorbing gases +! maximum number of absorbing gases integer, parameter :: MAXGAS = 7 -!> index upper limit of optical depth and transmittance tables +! index upper limit of optical depth and transmittance tables integer, parameter :: NTBMX = 10000 -!> SW bands counter starting index (for compatibility with previous +! SW bands counter starting index (for compatibility with previous !! SW radiation schemes) integer, parameter :: NSWSTR = 1 ! integer, parameter :: NSWEND = NBANDS integer, parameter :: NBDSW = NBANDS -!> \name The actual number of g-point for bands 16-29 +! \name The actual number of g-point for bands 16-29 integer :: NG16, NG17, NG18, NG19, NG20, NG21, NG22, & NG23, NG24, NG25, NG26, NG27, NG28, NG29 parameter ( NG16=06, NG17=12, NG18=08, NG19=08, NG20=10, @@ -155,7 +156,7 @@ module module_radsw_parameters ! data NG / NG16, NG17, NG18, NG19, NG20, NG21, NG22, & NG23, NG24, NG25, NG26, NG27, NG28, NG29 / -!> \name Accumulative starting index for bands 16-29 +! \name Accumulative starting index for bands 16-29 integer :: NS16, NS17, NS18, NS19, NS20, NS21, NS22, & NS23, NS24, NS25, NS26, NS27, NS28, NS29 parameter ( NS16=00, NS17=NS16+NG16, NS18=NS17+NG17, @@ -164,12 +165,12 @@ module module_radsw_parameters ! & NS25=NS24+NG24, NS26=NS25+NG25, NS27=NS26+NG26, & NS28=NS27+NG27, NS29=NS28+NG28 ) -!> array contains values of NS16-NS29 +! array contains values of NS16-NS29 integer, dimension(NBLOW:NBHGH) :: NGS data NGS / NS16, NS17, NS18, NS19, NS20, NS21, NS22, & & NS23, NS24, NS25, NS26, NS27, NS28, NS29 / -!> reverse checking of band index for each g-point +! reverse checking of band index for each g-point integer, dimension(NGPTSW) :: NGB data NGB(:) / 16,16,16,16,16,16, & ! band 16 & 17,17,17,17,17,17,17,17,17,17,17,17, & ! band 17 @@ -186,7 +187,7 @@ module module_radsw_parameters ! & 28,28,28,28,28,28, & ! band 28 & 29,29,29,29,29,29,29,29,29,29,29,29 / ! band 29 -!> \name Starting/ending wavenumber for each of the SW bands +! \name Starting/ending wavenumber for each of the SW bands real (kind=kind_phys), dimension(NBANDS):: wvnum1, wvnum2 data wvnum1(:) / & & 2600.0, 3251.0, 4001.0, 4651.0, 5151.0, 6151.0, 7701.0, & diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index 8d5e874ad..a31612c3a 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -6,8 +6,8 @@ !! @{ ! \defgroup NOAH_pre NOAH Land Surface Pre ! \ingroup NOAH -!! @{ -!! \brief Brief description of the parameterization +! @{ +! \brief Brief description of the parameterization module lsm_noah_pre contains @@ -36,9 +36,9 @@ end subroutine lsm_noah_pre_finalize !!| smcwlt2 | volume_fraction_of_condensed_water_in_soil_at_wilting_point | soil water fraction at wilting point | frac | 1 | real | kind_phys | inout | F | !!| smcref2 | threshold_volume_fraction_of_condensed_water_in_soil | soil moisture threshold | frac | 1 | real | kind_phys | inout | F | !! -!! \section general General Algorithm -!! \section detailed Detailed Algorithm -!! @{ +! \section general General Algorithm +! \section detailed Detailed Algorithm +! @{ subroutine lsm_noah_pre_run & & (im,km,drain,runof,evbs,evcw,trans,sbsno,snowc,snohf,smcwlt2, & & smcref2 & @@ -65,17 +65,17 @@ subroutine lsm_noah_pre_run & end subroutine lsm_noah_pre_run -!! @} +! @} end module lsm_noah_pre !! @} ! \defgroup NOAH_post NOAH Land Surface post ! \ingroup NOAH -!! @{ -!! \brief Brief description of the parameterization -!! \section diagram Calling Hierarchy Diagram -!! \section intraphysics Intraphysics Communication +! @{ +! \brief Brief description of the parameterization +! \section diagram Calling Hierarchy Diagram +! \section intraphysics Intraphysics Communication module lsm_noah_post contains @@ -88,7 +88,7 @@ end subroutine lsm_noah_post_finalize ! \brief Brief description of the subroutine ! -! \section arg_table_lsm_noah_post_run Arguments +!! \section arg_table_lsm_noah_post_run Arguments !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|--------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index 2b314e4b7..d4a5a5e9e 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -2,11 +2,6 @@ !! This file contains the GFS NSST model. !> \defgroup GFS_NSST GFS Near Sea Surface Temperature -!! @{ - module sfc_nst - - contains - !! \brief Near Sea Surface Temperature (NSST) is a temperature profile just below the sea surface. The GFS NSST scheme is used to forecast the NSST for two main purposes: supply SSTs to the atmospheric model for the calculation of air-sea heat and moisture fluxes and providing a sub-layer temperature profile forecast for use as a first guess in the Gridpoint Statistical Interpolator (GSI) data assimilation code. !! !! The GFS NSST scheme was initially developed at NCEP by Xu Li in 2007, and subsequently received contributions by S. Moorthi, Y.-T. Hu and J. Derber, leading to operational implementation in the GFS in 2017 (Li 2015 \cite Li_2015, and Li and Derber 2009 \cite Li_Derber_2009). The GFS NSST scheme predicts the vertical profile of sea temperature between the surface and a reference level (zr), which is on the order of 5 m. Only two physical process are considered in this scheme: diurnal thermocline layer warming and thermal skin layer (also known as sub-layer) cooling. All other process that could influence NSST are ignored in this simple scheme. @@ -32,6 +27,10 @@ module sfc_nst !! !! This space is reserved for a description of how this scheme uses information from other scheme types and/or how information calculated in this scheme is used in other scheme types. + module sfc_nst + + contains + ! \brief This subroutine is empty since there are no procedures that need to be done to initialize the GFS NSST code. !! This subroutine is empty since there are no procedures that need to be done to initialize the GFS NSST code. !! @@ -48,6 +47,7 @@ subroutine sfc_nst_finalize end subroutine sfc_nst_finalize !>\defgroup gfs_nst_main GFS sfc_nst Main +!!\ingroup GFS_NSST !> \brief This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. !! This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. !! \section arg_table_sfc_nst_run Argument Table @@ -120,7 +120,7 @@ end subroutine sfc_nst_finalize !! !! Under construction !! -!! @{ +!> @{ subroutine sfc_nst_run & & ( im, km, ps, u1, v1, t1, q1, tref, cm, ch, & & prsl1, prslki, islimsk, xlon, sinlat, stress, & @@ -690,7 +690,6 @@ subroutine sfc_nst_run & return end subroutine sfc_nst_run !> @} -!! @} end module sfc_nst @@ -927,6 +926,6 @@ subroutine sfc_nst_post_run & return end subroutine sfc_nst_post_run -!> @} +!! @} !! @} end module sfc_nst_post diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index cf0735b05..a5d3517a7 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -2,14 +2,14 @@ !! This file contains the GFS three level thermodynamic sea ice model. !> \defgroup GFS_Ice GFS Thermodynamics Sea Ice +!! \brief Three layer thermodynamic sea ice model based on M. Winton's +!! "a reformulated three-layer sea ice model", journal of atmospheric and oceanic technology, 2000. +!! \section diagram Calling Hierarchy Diagram +!! \section intraphysics Intraphysics Communication + module sfc_sice contains - -!! \brief Three layer thermodynamic sea ice model based on M. Winton's "a reformulated three-layer sea ice model", journal of atmospheric and oceanic technology, 2000. -!! \section diagram Calling Hierarchy Diagram -!! \section intraphysics Intraphysics Communication -!! !> \brief This subroutine is empty since there are no procedures that need to be done to initialize the GFS SICE code. !! \section arg_table_sice_init Argument Table !! @@ -73,7 +73,7 @@ end subroutine sfc_sice_finalize !! !! \section general General Algorithm !! \section detailed Detailed Algorithm -!! @{ +!> @{ subroutine sfc_sice_run & & ( im, km, ps, u1, v1, t1, q1, delt, & & sfcemis, dlwflx, sfcnsw, sfcdsw, srflag, & @@ -455,7 +455,6 @@ subroutine sfc_sice_run & !----------------------------------- !> \brief Brief description of the subroutine -!! subroutine ice3lay !................................... ! --- inputs: From cb99f0d54aa7e5bb3535c8415ae9968a8a195cab Mon Sep 17 00:00:00 2001 From: "Man.Zhang" Date: Tue, 23 Jan 2018 20:32:07 -0700 Subject: [PATCH 05/22] minor fix --- physics/GFS_calpreciptype.f90 | 20 +++++++++++++++++--- physics/mfdeepcnv.f | 3 +-- physics/mfshalcnv.f | 4 +--- physics/ozphys.f | 13 +++---------- 4 files changed, 22 insertions(+), 18 deletions(-) diff --git a/physics/GFS_calpreciptype.f90 b/physics/GFS_calpreciptype.f90 index 587af6d77..1f3da9afb 100644 --- a/physics/GFS_calpreciptype.f90 +++ b/physics/GFS_calpreciptype.f90 @@ -3,7 +3,16 @@ !! and its post. It is adopted from post but was made into a column to used by GFS model. !>\defgroup CALPRECIPTYPE GFS Dominant Precipitation Type -!! @{ +!!\brief This scheme contains the subroutine that calculates dominant +!! precipitation type and its post. It is adopted from post but was made +!! into a column to used by GFS model. +!! +!!\section diagram Calling Hierarchy Diagram +!! placeholder +!!\section intraphysics Intraphysics Communication +!! This space is reserved for a description of how this scheme uses info +!! from other scheme types and/or how information calculated in this +!! scheme is used in other scheme types. module GFS_calpreciptype contains @@ -13,6 +22,8 @@ subroutine GFS_calpreciptype_init end subroutine GFS_calpreciptype_init !>\defgroup gfs_calpreciptype GFS calpreciptype Main +!!\ingroup CALPRECIPTYPE +!!\brief blah blah !> \section arg_table_GFS_calpreciptype_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------|------------------------------------------------------------|---------|------|---------|-----------|--------|----------| @@ -44,6 +55,10 @@ end subroutine GFS_calpreciptype_init !! | srflag | flag_for_precipitation_type | snow(1)/rain(0) flag for precipitation | flag | 1 | real | kind_phys | out | F | !! | tprcp | nonnegative_lwe_thickness_of_precipitation_amount_on_dynamics_timestep | nonnegative precipitation amount in one dynamics time step | m | 1 | real | kind_phys | out | F | !! +!! \section general General Algorithm +!! +!! \section detailed Detailed Algorithm +!! @{ subroutine GFS_calpreciptype_run(kdt,nrcm,im,ix,lm,lp1,randomno, & cal_pre, & gt0,gq0,prsl,prsi, rainc,frain,rain1, & @@ -311,6 +326,7 @@ subroutine GFS_calpreciptype_run(kdt,nrcm,im,ix,lm,lp1,randomno, & return end subroutine GFS_calpreciptype_run +!! @} ! !&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& ! @@ -1522,5 +1538,3 @@ subroutine GFS_calpreciptype_finalize end subroutine GFS_calpreciptype_finalize end module GFS_calpreciptype - -!! @} diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index ef6067f46..e71b93ea1 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -53,8 +53,7 @@ !! to more strongly suppress convection in a drier environment. !! !! \section diagram Calling Hierarchy Diagram -!! \image html SAMF_Flowchart.png "Diagram depicting how the SAMF deep convection -!! scheme is called from the FV3GFS physics time loop" height=2cm +!! !! \section intraphysics Intraphysics Communication !! This space is reserved for a description of how this scheme uses information !! from other scheme types and/or how information calculated in this scheme diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index b141faf3e..3a4d9d238 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -23,9 +23,7 @@ !! are described in Han et al. (2017) \cite han_et_al_2017 . !! !! \section diagram Calling Hierarchy Diagram -!! \image html SAMF_shal_Flowchart.png "Diagram depicting how the SAMF -!! shallow convection scheme is called from the FV3GFS physics time loop" -!! height=2cm +!! !! \section intraphysics Intraphysics Communication !! This space is reserved for a description of how this scheme uses !! information from other scheme types and/or how information calculated diff --git a/physics/ozphys.f b/physics/ozphys.f index 635248c4d..95f67b203 100644 --- a/physics/ozphys.f +++ b/physics/ozphys.f @@ -12,12 +12,10 @@ !! Original version of these terms were provided by NASA/DAO based on !! NASA 2D Chemistry model - GSM is capable of running both versions !! +!! \section diagram Calling Hierarchy Diagram !! \section intra_oz Intraphysics Communication !! -!! @{ - module ozphys_pre - contains ! \section arg_table_ozphys_pre_init Argument Table @@ -41,8 +39,6 @@ end subroutine ozphys_pre_finalize end module ozphys_pre - - module ozphys contains @@ -55,6 +51,7 @@ subroutine ozphys_init() end subroutine ozphys_init !>\defgroup GFS_ozphys GFS ozphys Main +!>\ingroup GFS_ozn !! \brief This is the main subroutine !! \section arg_table_ozphys_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -197,7 +194,6 @@ subroutine ozphys_run ( & ! return end subroutine ozphys_run -!! @} !> @} ! \brief Brief description of the subroutine @@ -207,12 +203,9 @@ end subroutine ozphys_run subroutine ozphys_finalize() end subroutine ozphys_finalize - end module ozphys - - module ozphys_post contains @@ -223,7 +216,7 @@ subroutine ozphys_post_init() end subroutine ozphys_post_init -!! \section arg_table_ozphys_post_run Argument Table +! \section arg_table_ozphys_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|----------------------------------------------|----------------------------------------------|---------|------|----------------------------|-----------|--------|----------| !! | ix | horizontal_dimension | horizontal dimension | count | 0 | integer | | in | F | From 39be11b9c4bafb9c9cfba1b3b24d25da919cc7a3 Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Thu, 25 Jan 2018 10:16:54 -0700 Subject: [PATCH 06/22] format cleanup --- physics/docs/ccpp_dox | 2 +- physics/docs/img/schematic_sice.png | Bin 0 -> 23228 bytes physics/docs/img/sice_wonton2000_fig1.png | Bin 0 -> 142025 bytes physics/docs/library.bib | 121 +++++++++++++++++++--- physics/docs/txt/mainpage.txt | 1 - physics/gscond.f | 8 +- physics/gwdc.f | 11 +- physics/gwdps.f | 8 +- physics/mfdeepcnv.f | 8 +- physics/mfshalcnv.f | 6 +- physics/moninedmf.f | 6 +- physics/ozphys.f | 4 +- physics/radlw_main.f | 7 ++ physics/sfc_diff.f | 10 +- physics/sfc_drv.f | 58 ++++++++--- physics/sfc_nst.f | 6 +- physics/sfc_sice.f | 69 ++++++++++-- physics/sflx.f | 43 ++++++++ 18 files changed, 302 insertions(+), 66 deletions(-) create mode 100644 physics/docs/img/schematic_sice.png create mode 100644 physics/docs/img/sice_wonton2000_fig1.png diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index 2aa09a7b3..4b5a08bfe 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -123,9 +123,9 @@ INPUT = txt/mainpage.txt \ ### Microphysics ../precpd.f \ ../gscond.f \ - ../GFS_calpreciptype.f90 \ ### Land Surface ../sfc_drv.f \ + ../sflx.f \ ../sfc_diff.f \ ### Sea Ice Surface ../sfc_sice.f \ diff --git a/physics/docs/img/schematic_sice.png b/physics/docs/img/schematic_sice.png new file mode 100644 index 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file was created using BibDesk. %% http://bibdesk.sourceforge.net/ -%% Created for Man Zhang at 2016-10-11 14:56:34 -0600 +%% Created for Man Zhang at 2018-01-25 08:40:47 -0700 %% Saved with string encoding Unicode (UTF-8) +@article{chen_et_al_1997, + Author = {F. Chen and Z. Janjic and K. Mitchell}, + Date-Added = {2018-01-25 03:23:50 +0000}, + Date-Modified = {2018-01-25 03:26:47 +0000}, + Journal = {Boundary-Layer Meteorology}, + Number = {3}, + Pages = {391-421}, + Title = {Impact of atmospheric surface-layer parameterizations in the new land-surface scheme of the NCEP mesoscale Eta model }, + Volume = {85}, + Year = {1997}} + +@article{winton_2000, + Author = {M. Winton}, + Date-Added = {2018-01-24 21:34:39 +0000}, + Date-Modified = {2018-01-24 21:41:05 +0000}, + Journal = {J. Atmos. Oceanic Tech.}, + Pages = {525-531}, + Title = {A reformulated three-layer sea ice model}, + Volume = {17}, + Year = {2000}} + +@phdthesis{Lim_2011, + Address = {Seoul, South Korea}, + Author = {K.-S. S. Lim}, + Date-Added = {2018-01-24 18:58:17 +0000}, + Date-Modified = {2018-01-24 18:59:50 +0000}, + School = {Yonsei University}, + Title = {Investigation of aerosol indirect effects on simulated moist convections.}, + Year = {2011}} + +@article{arakawa_and_wu_2013, + Author = {A. Arakawa and C.-M. Wu}, + Date-Added = {2018-01-24 18:54:08 +0000}, + Date-Modified = {2018-01-24 18:57:10 +0000}, + Journal = {J. Atmos. Sci.}, + Pages = {1977-1992}, + Title = {A unified representation of deep moist convection in numerical modeling of the atmosphere. Part I}, + Volume = {70}, + Year = {2013}} + +@article{han_et_al_2017, + Author = {J. Han and W. Wang and Y. C. Kwon and S.-Y. Hong and V. Tallapragada and F. Yang}, + Date-Added = {2018-01-24 18:48:52 +0000}, + Date-Modified = {2018-01-24 18:53:21 +0000}, + Journal = {Weather and Forecasting}, + Pages = {2005-2017}, + Title = {Updates in the NCEP GFS cumulus convective schemes with scale and aerosol awareness}, + Volume = {32}, + Year = {2017}} + +@article{grell_and_freitas_2014, + Author = {G.A. Grell and S.R. Freitas}, + Date-Added = {2018-01-24 18:44:56 +0000}, + Date-Modified = {2018-01-24 18:47:21 +0000}, + Journal = {Atmos. Chem. Phys.}, + Pages = {5233-5250}, + Title = {A scale and aerosol aware stochastic convective parameterization for weather and air quality modeling}, + Volume = {14}, + Year = {2014}} + +@article{Koren_et_al_1999, + Author = {V. Koren and J. Schaake and K. Mitchell and Q.-Y. Duan and F. Chen and J. Baker}, + Date-Added = {2018-01-24 18:41:34 +0000}, + Date-Modified = {2018-01-24 18:43:55 +0000}, + Journal = {J. Geophys. Res.}, + Number = {D16}, + Pages = {19569-19585}, + Title = {A parameterization of snowpack and frozen ground intended for NCEP weather and climate models}, + Volume = {104}, + Year = {1999}} + +@article{ek_et_al_2003, + Author = {M. B. Ek and K. E. Mitchell and Y. Lin and E. Rogers and P. Grunmann and V. Koren and G. Gayno and J. D. Tarpley}, + Date-Added = {2018-01-24 18:35:48 +0000}, + Date-Modified = {2018-01-24 18:39:48 +0000}, + Journal = {J. Geophys. Res.}, + Number = {D22}, + Pages = {8851}, + Title = {Implementation of Noah land-surface model advances in the NCEP operational mesoscale Eta model}, + Volume = {108}, + Year = {2003}} + +@article{chen_et_al_1996, + Author = {F. Chen and K. Mitchell and J. Schaake and Y. Xue and H.-L. Pan and V. Koren and Q.-Y. Duan and M. Ek and A. Betts}, + Date-Added = {2018-01-24 18:31:48 +0000}, + Date-Modified = {2018-01-24 18:35:18 +0000}, + Journal = {J. Geophys. Res.}, + Number = {D3}, + Pages = {7251-7268}, + Title = {Modeling of land-surface evaporation by four schemes and comparison with observations}, + Volume = {101}, + Year = {1996}} + @article{raisanen_and_barker_2004, Author = {P. Raisanen and H.W. Barker}, Date-Added = {2016-10-11 20:51:22 +0000}, @@ -60,22 +153,24 @@ @article{king_and_harshvardhan_1986 Year = {1986}} @url{Li_2015, - Author = {Xu Li}, - Title = {The development of the NSST within the NCEP GFS/CFS}, - Url = {http://cpo.noaa.gov/sites/cpo/MAPP/workshops/rtf_technical_ws/presentations/21_Xu_Li.pdf}} + Author = {Xu Li}, + Title = {The development of the NSST within the NCEP GFS/CFS}, + Url = {http://cpo.noaa.gov/sites/cpo/MAPP/workshops/rtf_technical_ws/presentations/21_Xu_Li.pdf}, + Bdsk-Url-1 = {http://cpo.noaa.gov/sites/cpo/MAPP/workshops/rtf_technical_ws/presentations/21_Xu_Li.pdf}} @url{Li_Derber_2009, - Author = {Xu Li and John Derber}, - Title = {Near Sea Surface Temperatures (NSST) Analysis in NCEP GFS}, - Url = {https://www.jcsda.noaa.gov/documents/meetings/wkshp2008/4/JCSDA_2008_Li.pdf}} + Author = {Xu Li and John Derber}, + Title = {Near Sea Surface Temperatures (NSST) Analysis in NCEP GFS}, + Url = {https://www.jcsda.noaa.gov/documents/meetings/wkshp2008/4/JCSDA_2008_Li.pdf}, + Bdsk-Url-1 = {https://www.jcsda.noaa.gov/documents/meetings/wkshp2008/4/JCSDA_2008_Li.pdf}} @article{Fairall_all_1996, - Author = {C. W. Fairall and E. F. Bradley and J. S. Godfrey and G. A. Wick and J. B. Edson and G. S. Young}, - Journal = {J. Geophys. Res.}, - Pages = {1295-1308}, - Title = {Cool-skin and warm-layer effects on sea surface temperature}, - Volume = {101(C1)}, - Year = {1996}} + Author = {C. W. Fairall and E. F. Bradley and J. S. Godfrey and G. A. Wick and J. B. Edson and G. S. Young}, + Journal = {J. Geophys. Res.}, + Pages = {1295-1308}, + Title = {Cool-skin and warm-layer effects on sea surface temperature}, + Volume = {101(C1)}, + Year = {1996}} @url{key_2002, Address = {Madison, Wisconsin}, diff --git a/physics/docs/txt/mainpage.txt b/physics/docs/txt/mainpage.txt index 6410a3b3a..30ba3eb56 100644 --- a/physics/docs/txt/mainpage.txt +++ b/physics/docs/txt/mainpage.txt @@ -14,5 +14,4 @@ The documentation found here corresponds to the state of the operational GFS phy - \ref GFS_ogwd - \ref GFS_cgwd - \ref GFS_ozn - - \ref CALPRECIPTYPE */ diff --git a/physics/gscond.f b/physics/gscond.f index 31f2040b0..5ae090b7c 100644 --- a/physics/gscond.f +++ b/physics/gscond.f @@ -36,7 +36,13 @@ module GFS_zhaocarr_gscond !! conversion from condensate (water and ice) to precipitation !! - EVPCO: Coefficient for evaporation of precipitation !! -!! \section intramps Intraphysics Communication +!! \section diagram Calling Hierarchy Diagram +!! +!! \todo zhao-carr calling hierarchy diagram +!! +!! \section intraphysics Intraphysics Communication +!! \todo zhao-carr intraphysics communication + !> \defgroup condense Grid-Scale Condensation and Evaporation of Cloud !! @{ diff --git a/physics/gwdc.f b/physics/gwdc.f index c48f335ba..21b80bba2 100644 --- a/physics/gwdc.f +++ b/physics/gwdc.f @@ -61,13 +61,14 @@ !! positive effects from using the parameterization are seen in the !! tropical upper troposphere and lower stratosphere. !! -!!\section intra_gwdps Intraphysics Communication -!! - Routine GWDC is called from GBPHYS after call -!! to SASCNVN - +!> \section diagram Calling Hierarchy Diagram +!! +!! \todo gwdc calling hierarchy diagram +!! +!> \section intraphysics Intraphysics Communication +!! \todo gwdc calling hierarchy diagram module gwdc_pre - contains ! \brief Brief description of the subroutine diff --git a/physics/gwdps.f b/physics/gwdps.f index 22d78c636..7165c697e 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -95,7 +95,13 @@ !! four times stronger mountain blocking and one half the strength of !! gravity wave drag than the T383L64 version. !! -!!\section intra_gwdps Intraphysics Communication +!> \section diagram Calling Hierarchy Diagram +!! +!! \todo gwdps calling hierarchy diagram +!! +!> \section intraphysics Intraphysics Communication +!! \todo gwdps interaphysics communication + module gwdps_pre diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index e71b93ea1..00db6808e 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -53,8 +53,9 @@ !! to more strongly suppress convection in a drier environment. !! !! \section diagram Calling Hierarchy Diagram -!! +!! \todo mfdeepcnv calling hierarchy diagram !! \section intraphysics Intraphysics Communication +!! \todo mfshalcnv intraphysics diagram !! This space is reserved for a description of how this scheme uses information !! from other scheme types and/or how information calculated in this scheme !! is used in other scheme types. @@ -63,11 +64,6 @@ module sasas_deep contains - -!! \brief Brief description of the parameterization -!! \section diagram Calling Hierarchy Diagram -!! \section intraphysics Intraphysics Communication - ! \brief Brief description of the subroutine ! ! \section arg_table_sasasdeep_init Argument Table diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 3a4d9d238..2ac467113 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -23,11 +23,9 @@ !! are described in Han et al. (2017) \cite han_et_al_2017 . !! !! \section diagram Calling Hierarchy Diagram -!! +!! \todo mfshalcnv calling hierarchy diagram !! \section intraphysics Intraphysics Communication -!! This space is reserved for a description of how this scheme uses -!! information from other scheme types and/or how information calculated -!! in this scheme is used in other scheme types. +!! \todo mfshalcnv intraphysics communitcation module sasas_shal contains diff --git a/physics/moninedmf.f b/physics/moninedmf.f index bb6d3f6c9..ec0fb4bb0 100644 --- a/physics/moninedmf.f +++ b/physics/moninedmf.f @@ -13,9 +13,9 @@ module edmf !! The PBL scheme's main task is to calculate tendencies of temperature, moisture, and momentum due to vertical diffusion throughout the column (not just the PBL). The scheme is an amalgamation of decades of work, starting from the initial first-order PBL scheme of Troen and Mahrt (1986) \cite troen_and_mahrt_1986, implemented according to Hong and Pan (1996) \cite hong_and_pan_1996 and modified by Han and Pan (2011) \cite han_and_pan_2011 and Han et al. (2015) \cite han_et_al_2015 to include top-down mixing due to stratocumulus layers from Lock et al. (2000) \cite lock_et_al_2000 and replacement of counter-gradient terms with a mass flux scheme according to Siebesma et al. (2007) \cite siebesma_et_al_2007 and Soares et al. (2004) \cite soares_et_al_2004. Recently, heating due to TKE dissipation was also added according to Han et al. (2015) \cite han_et_al_2015. !! !! \section diagram Calling Hierarchy Diagram -!! \image html Hybrid_EDMF_Flowchart.png "Diagram depicting how the Hybrid EDMF PBL scheme is called from the GSM physics time loop" height=2cm +!! \todo pbl calling hierarchy diagram !! \section intraphysics Intraphysics Communication -!! This space is reserved for a description of how this scheme uses information from other scheme types and/or how information calculated in this scheme is used in other scheme types. +!! \todo pbl intraphysics communication subroutine edmf_init () end subroutine edmf_init @@ -28,7 +28,7 @@ end subroutine edmf_finalize !! !! The scheme works on a basic level by calculating background diffusion coefficients and updating them according to which processes are occurring in the column. The most important difference in diffusion coefficients occurs between those levels in the PBL and those above the PBL, so the PBL height calculation is of utmost importance. An initial estimate is calculated in a "predictor" step in order to calculate Monin-Obukhov similarity values and a corrector step recalculates the PBL height based on updated surface thermal characteristics. Using the PBL height and the similarity parameters, the diffusion coefficients are updated below the PBL top based on Hong and Pan (1996) \cite hong_and_pan_1996 (including counter-gradient terms). Diffusion coefficients in the free troposphere (above the PBL top) are calculated according to Louis (1979) \cite louis_1979 with updated Richardson number-dependent functions. If it is diagnosed that PBL top-down mixing is occurring according to Lock et al. (2000) \cite lock_et_al_2000 , then then diffusion coefficients are updated accordingly. Finally, for convective boundary layers (defined as when the Obukhov length exceeds a threshold), the counter-gradient terms are replaced using the mass flux scheme of Siebesma et al. (2007) \cite siebesma_et_al_2007 . In order to return time tendencies, a fully implicit solution is found using tridiagonal matrices, and time tendencies are "backed out." Before returning, the time tendency of temperature is updated to reflect heating due to TKE dissipation following Han et al. (2015) \cite han_et_al_2015 . !! -!! \section arg_table_edmf_run +!! \section arg_table_edmf_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------------------------|-------------------------------------------------------|---------------|------|---------|-----------|--------|----------| !! | ix | horizontal_dimension | horizontal dimension | count | 0 | integer | | in | F | diff --git a/physics/ozphys.f b/physics/ozphys.f index 95f67b203..5c5d101f8 100644 --- a/physics/ozphys.f +++ b/physics/ozphys.f @@ -2,7 +2,7 @@ !! This file is ozone sources and sinks. !> \defgroup GFS_ozn GFS Ozone Sources and Sinks -!! \detail The operational GFS currently parameterizes ozone production and +!! \brief The operational GFS currently parameterizes ozone production and !! destruction based on monthly mean coefficients provided by Naval !! Research Laboratory through CHEM2D chemistry model !! (McCormack et al. 2006 \cite mccormack_et_al_2006). @@ -13,7 +13,9 @@ !! NASA 2D Chemistry model - GSM is capable of running both versions !! !! \section diagram Calling Hierarchy Diagram +!! \todo ozphys calling hierarchy diagram !! \section intra_oz Intraphysics Communication +!! \todo ozphys intraphysics communication !! module ozphys_pre contains diff --git a/physics/radlw_main.f b/physics/radlw_main.f index 466f5ca1e..8cb1d7a68 100644 --- a/physics/radlw_main.f +++ b/physics/radlw_main.f @@ -90,6 +90,13 @@ !! the lower atmosphere (<3km) a monthly mean CO2 distribution in 15 !! degree horizontal resolution is used, while a global mean monthly !! value is used in the upper atmosphere. +!! +!> \section diagram Calling Hierarchy Diagram +!! \todo RRTMG calling hierarchy diagram +!! +!> \section intraphysics Intraphysics Communication +!! \todo RRTMG intraphysics communication + ! !!!!! ============================================================== !!!!! !!!!! lw-rrtm3 radiation package description !!!!! diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index 822c1ac26..6b991ab6c 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -3,9 +3,11 @@ !> \defgroup Sfc_ex_cal GFS Surface Exchange Coefficient Calculation !! @{ -!! \brief Brief description of the scheme +!! \brief This is the first subroutine called in surface layer loop to calculate surface exchange ciefficients and near-surface wind. !! \section diagram Calling Hierarchy Diagram +!! \todo sfc_diff Calling hierarchy diagram !! \section intraphysics Intraphysics Communication +!! \todo sfc_diff intraphysics communication module surface_exchange_coefficients contains @@ -20,8 +22,8 @@ end subroutine sfc_ex_coef_finalize !> \defgroup GFS_diff_main GFS sfc_diff Main !! \ingroup Sfc_ex_cal -!> \brief Brief description of the subroutine -!! \section arg_table_sfc_ex_coef_run Arguments +!> \brief This is the first subroutine called in surface layer loop to calculate surface exchange coefficients and near-surface wind. +!! \section arg_table_sfc_ex_coef_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|-------------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -57,7 +59,9 @@ end subroutine sfc_ex_coef_finalize !!| redrag | flag_for_reduced_drag_coefficient_over_sea | flag for reduced drag coefficient over sea | flag | 0 | logical | | in | F | !! !! \section general General Algorithm +!! \todo sfc_ex_coef_run general algorithm !! \section detailed Detailed Algorithm +!! \todo sfc_ex_coef_run Detailed Algorithm !! @{ subroutine sfc_ex_coef_run & & (im,ps,u1,v1,t1,q1,z1, & diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index a31612c3a..5122150d8 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -1,9 +1,44 @@ !> \file sfc_drv.f -!! This file contains the NOAH land surface scheme. +!! This file contains the NOAH land surface scheme driver. !> \defgroup NOAH GFS NOAH Land Surface Scheme -!! \brief This is the NOAH land surface scheme. -!! @{ +!! \brief The Noah LSM(version 2.7) is the land model. +!! +!! In 2005, the NCEP Noah LSM (Version 2.7.1) replaced +!! the Oregon State University (OSU) LSM, which had been operational in the GFS since +!! the mid-1990s. The Noah LSM embodies about 10 years of upgrades (see Chen et.al. 1996 +!! \cite chen_et_al_1996; Koren et. al. 1999 \cite koren_et_al_1999; Ek et. al. 2003 +!! \cite ek_et_al_2003) to its ancestor, the OSU LSM. +!! +!! The Noah LSM upgrade includes an increase from two (10, 190 cm thick) to four +!! soil layers (10, 30, 60, 100 cm thick). addition of frozen soil physics, new +!! formulations for infiltration and runoff (giving more runoff for unsaturated +!! soils), revised physics of the snowpack and its influence on surface heat fluxes +!! and albedo, tuning and adding canopy resistance parameters, allowing spatially +!! varying root depth, revised treatment of ground heat flux and soil thermal +!! conductivity, reformulation of dependence of direct surface evaporation on first +!! layer soil moisture, and improved seasonality of green vegetation cover. The +!! frozen soil physics includes soil heat sinks/sources from freezing/thawing +!! and influences vertical transport of soil moisture, soil thermal conductivity +!! and heat capacity, and present prognostic states of snowpack water-equivalent (SWE), +!! total soil moisture (liquid plus frozen), soil temperature, canopy water, and skin +!! temperature. SWE divided by the snowpack depth gives the snowpack density. Total +!! soil moisture minus liquid soil moisture gives the frozen soil moisture. +!! +!! To provide initial values of soil moisture/temperature, the Noah LSM land states +!! cycle continuous in the coupled atmosphere/land global model of the GDAS. These +!! land states respond to the global model's predicted land-surface forcing (precipitation, +!! surface radiation, near-surface air temperature, humidity, and wind speed). Since +!! the land component of the GDAS is forced by model prediction rather than observed +!! precipitation, we avoid undue drift by nudging soil moisture towards a monthly +!! global climatology(in GDAS only, not in forecast). +!! +!! +!!\section diagram Calling Hierarchy Diagram +!! \todo NOAH calling hierarchy diagram +!!\section Intraphysics Intraphysics Communication +!! \todo NOAH intraphysics communication +!! ! \defgroup NOAH_pre NOAH Land Surface Pre ! \ingroup NOAH ! @{ @@ -20,7 +55,7 @@ end subroutine lsm_noah_pre_finalize ! \brief Brief description of the subroutine ! -! \section arg_table_lsm_noah_pre_run Arguments +! \section arg_table_lsm_noah_pre_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|--------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -88,7 +123,7 @@ end subroutine lsm_noah_post_finalize ! \brief Brief description of the subroutine ! -!! \section arg_table_lsm_noah_post_run Arguments +!! \section arg_table_lsm_noah_post_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|--------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -248,16 +283,12 @@ end subroutine lsm_noah_finalize !----------------------------------- ! subroutine sfc_drv & -!> \defgroup NOAH_main GFS sfc_drv Main +!> \defgroup NOAH_drv GFS sfc_drv Main !! \ingroup NOAH !! @{ -!! \brief Brief description of the parameterization -!! \section diagram Calling Hierarchy Diagram -!! \section intraphysics Intraphysics Communication - -!> \brief Brief description of the subroutine +!! \brief This is NOAH LSM driver scheme. !! -!! \section arg_table_lsm_noah_run Arguments +!! \section arg_table_lsm_noah_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|------------------------------------------------------------------------------|-----------------------------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -325,7 +356,9 @@ end subroutine lsm_noah_finalize !!| wet1 | normalized_soil_wetness | normalized soil wetness | frac | 1 | real | kind_phys | out | F | !! !! \section general General Algorithm +!! \todo sfc_drv general algorithm !! \section detailed Detailed Algorithm +!! \todo sfc_drv detailed algorithm !! @{ subroutine lsm_noah_run & & ( im, km, ps, u1, v1, t1, q1, soiltyp, vegtype, sigmaf, & @@ -772,4 +805,3 @@ end subroutine lsm_noah_run end module lsm_noah !! @} -!! @} diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index d4a5a5e9e..bccd7d2b9 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -48,8 +48,8 @@ end subroutine sfc_nst_finalize !>\defgroup gfs_nst_main GFS sfc_nst Main !!\ingroup GFS_NSST -!> \brief This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. -!! This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. +!> \brief This is the second subroutine called in surface land loop. +!!This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. !! \section arg_table_sfc_nst_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------------|-------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| @@ -118,7 +118,7 @@ end subroutine sfc_nst_finalize !! !! \section NSST_detailed_algorithm !! -!! Under construction +!! \todo nsst detailed algorithm !! !> @{ subroutine sfc_nst_run & diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index a5d3517a7..74681977c 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -1,30 +1,76 @@ !> \file sfc_sice.f !! This file contains the GFS three level thermodynamic sea ice model. -!> \defgroup GFS_Ice GFS Thermodynamics Sea Ice -!! \brief Three layer thermodynamic sea ice model based on M. Winton's -!! "a reformulated three-layer sea ice model", journal of atmospheric and oceanic technology, 2000. +!> \defgroup GFS_Ice GFS Three-layer Thermodynamics Sea Ice +!! \brief This is three-layer thermodynomics sea-ice model based on Winton (2000) \cite winton_2000. +!! +!! Sea ice is a thin skin of frozen water covering the polar oceans. The sea ice strongly interacts with both the atmosphere above and the ocean underneath in the high +!! latitudes. In a coupled weather/climate system, changes in sea ice extent, thickness and concentration +!! regionally or globally would influence oceanic and atmospheric conditions, which in turn affect the +!! sea ice distribution. The physical and dynamical processes affecting the weather and climate are +!! considered as follows. +!! +!! The high albedo of the sea ice reflects more solar radiation back to the space. The feedbacks are +!! considered as positive. The broader the sea ice cover, the higher the surface albedo, which result +!! in less amount of solar radiation absorbed at the Earth's surface. A cooler surface would favor more +!! sea ice to form. The process would be reversed in less sea ice situation. +!! +!! The sea ice restricts the heat/water exchange between the air and ocean. The presence of extensive +!! areas of sea ice would suppress the heat loss in winter and the heat gain in summer by the ocean. +!! Even a thin ice cover influences the turbulent heat transfer significantly between ocean and +!! atmosphere. The surface fluxes of sensible and latent heat can be greater by up to two orders of magnitude +!! at the open water surface of a lead or polynya than that through (snow covered) pack ice. +!! +!! The sea ice modifies air/sea momentum transfer, ocean fresh water balance and ocean circulation. +!! The freezing and melting of the ocean surface and the associated fluxes of salt and heat produce major +!! changes in the density structure of the polar water. Formation of sea ice injects salt into the ocean +!! makes the water heavier and more convectively unstable, conversely when melting occurs, stable and fresh +!! layers can prevent deep covective activity. +!! +!! A sea ice model, in general, may contain subcomponents treating 1)dynamics (ice motion), +!! 2)ice transport, 3) multiple ice thickness categories (including leads), 4) surface albedo, +!! and 5) vertical thermodynamics. GFS sea ice scheme is concerned with a scheme for the +!! last of these processes. +!! +!! A three-layer thermodynamic sea ice model has been coupled to NCEP GFS. It predicts sea ice/snow thickness, +!! the surface temperature and ice temperature structure. In each model grid box, the heat and moisture +!! fluxes and albedo are treated separately for the ice and the open water. +!! +!!\image html sice_wonton2000_fig1.png "Fig.1 Schematic representation of the three-layer model" width=5cm +!! The model has four prognostic variables: the snow layer thickness \f$h_s\f$, the ice layer thickness +!! \f$h_i\f$, the upper and lower ice layer temperatures located at the midpoints of the layers +!! \f$h_i/4\f$ and \f$3h_i/4\f$ below the ice surface, respectively \f$T_1\f$ and \f$T_2\f$. The temperature of +!! the bottom of the ice is fixed at \f$T_f\f$, the freezing temperature of seawater. The temperature of +!! the top of the ice or snow, \f$T_s\f$, is determined from the surface energy balance. +!! +!! The model consists of a zero-heat-capacity snow layer overlying two equally thick sea ice layers (Fig.1). +!! The upper ice layer has a variable heat capacity to represent brine pockets. +!! +!! !! \section diagram Calling Hierarchy Diagram +!! !! \section intraphysics Intraphysics Communication +!!\image html schematic_sice.png "Fig.2 NCEP Sea Ice Model System Diagram" width=10cm module sfc_sice contains -!> \brief This subroutine is empty since there are no procedures that need to be done to initialize the GFS SICE code. -!! \section arg_table_sice_init Argument Table -!! + +! \brief This subroutine is empty since there are no procedures that need to be done to initialize the GFS SICE code. +! \section arg_table_sice_init Argument Table +! subroutine sfc_sice_init end subroutine sfc_sice_init !! -!> \brief This subroutine is empty since there are no procedures that need to be done to finalize the GFS SICE code. -!! \section arg_table_sice_finalize Argument Table -!! +! \brief This subroutine is empty since there are no procedures that need to be done to finalize the GFS SICE code. +! \section arg_table_sice_finalize Argument Table +! subroutine sfc_sice_finalize end subroutine sfc_sice_finalize !>\defgroup gfs_sice_main GFS sfc_sice Main -!> \brief blah blah +!> \todo gfs_sice_main brief blah blah !! @{ !! \ingroup GFS_Ice !! \section arg_table_sfc_sice_run Arguments @@ -454,7 +500,8 @@ subroutine sfc_sice_run & !> @} !----------------------------------- -!> \brief Brief description of the subroutine +!> This subroutine is the entity of three-layer sea ice vertical thermodynamics +!! based on Winton(2000) \cite winton_2000 . subroutine ice3lay !................................... ! --- inputs: diff --git a/physics/sflx.f b/physics/sflx.f index 20b4b60f5..19b67ffd5 100644 --- a/physics/sflx.f +++ b/physics/sflx.f @@ -1,3 +1,19 @@ +!\file sflx.f +!! This file contains the NCEP Noah LSM (Version 2.7.1) + +!>\defgroup NOAH_LSM NCEP Noah LSM +!!\ingroup NOAH_drv +!!\brief This is sub-driver for "NOAH/OSU LSM" family of physics subroutines. +!! It is a soil/veg/snowpack land-surface model to update soil moisture, soil +!! ice, soil temperature, skin temperature, snowpack water content, snowdepth, +!! and all terms of the surface energy balance and surface water balance +!! (excluding input atmospheric forcings of downward radiation and precip). +!! +!!\section general General Algorithm +!!\todo NOAH LSM general algorithm +!!\section detailed Detailed Algorithm +!!\todo NOAH LSM detailed algorithm +!! @{ !----------------------------------- subroutine sflx & !................................... @@ -781,6 +797,7 @@ subroutine sflx & !*************************************! !----------------------------------- +!>This subroutine calculates albedo including snow effect (0 -> 1). subroutine alcalc !................................... ! --- inputs: @@ -863,6 +880,10 @@ end subroutine alcalc !----------------------------------- +!> This subroutine calculates canopy resistance which depends on incoming +!! solar radiation, air temperature, atmospheric water vapor pressure +!! deficit at the lowest model level, and soil moisture (preferably unfrozen +!! soil moisture rather than total). subroutine canres !................................... ! --- inputs: @@ -1017,6 +1038,7 @@ end subroutine canres !----------------------------------- +!> This subroutine calculates snow termal conductivity subroutine csnow !................................... ! --- inputs: @@ -1078,6 +1100,9 @@ end subroutine csnow !----------------------------------- +!> This subroutine calculates soil moisture and heat flux values and +!! update soil moisture content and soil heat content values for the +!! case when now snow pack is present. subroutine nopac !................................... ! --- inputs: @@ -1341,6 +1366,9 @@ end subroutine nopac !----------------------------------- +!> This subroutine calculates potential evaporation for the current point. +!! various partial sums/products are also calculated and passed back +!! to the calling routine for later use subroutine penman !................................... ! --- inputs: @@ -1447,6 +1475,9 @@ end subroutine penman !----------------------------------- +!> This subroutine internally sets default values or optionally read-in +!! via namelist i/o, all soil and vegetation parateters requied for the execusion +!! of the NOAH LSM. subroutine redprm !................................... ! --- inputs: @@ -1736,6 +1767,8 @@ end subroutine redprm !----------------------------------- +!> This subroutine calculates surface layer exchange coefficients +!! via iterative process(see chen et al. 1997 \cite chen_et_al_1997). subroutine sfcdif !................................... ! --- inputs: @@ -2021,6 +2054,7 @@ end subroutine sfcdif !----------------------------------- +!> This subroutine calculates snow fraction (0->1). subroutine snfrac !................................... ! --- inputs: @@ -2090,6 +2124,9 @@ end subroutine snfrac !----------------------------------- +!> This subroutine calculates soil moisture and heat flux values and +!! update soil moisture content and soil heat content values for the +!! case when a snow pack is present. subroutine snopac !................................... ! --- inputs: @@ -2605,6 +2642,8 @@ end subroutine snopac !----------------------------------- +!> This subroutine calculates snow depth and densitity to account +!! for the new snowfall. new values of snow depth & density returned. subroutine snow_new !................................... ! --- inputs: @@ -2677,6 +2716,7 @@ end subroutine snow_new !----------------------------------- +!> This subroutine calculates total roughness length over snow. subroutine snowz0 !................................... ! --- inputs: @@ -2727,6 +2767,8 @@ end subroutine snowz0 !----------------------------------- +!> This subroutine calculates thermal diffusivity and conductivity +!! of the soil for a given point and time. subroutine tdfcnd & !................................... ! --- inputs: @@ -5471,3 +5513,4 @@ end subroutine wdfcnd !................................... end subroutine sflx !----------------------------------- +!! @} From 89c9fcf210a14cebfd973341d10b74d3ac260956 Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Fri, 2 Feb 2018 15:22:38 -0700 Subject: [PATCH 07/22] improve documentation and add figures. --- physics/GFS_calpreciptype.f90 | 17 +- physics/GFS_surface_loop_control.f | 2 - physics/docs/ccpp_dox | 5 + physics/docs/img/GFS_sice_wonton2000_fig1.png | Bin 0 -> 99143 bytes physics/docs/img/Noah_LA_interaction.png | Bin 0 -> 345183 bytes physics/docs/img/land_dataset.png | Bin 0 -> 435539 bytes physics/docs/img/roughness_length_fig1.png | Bin 0 -> 382306 bytes physics/docs/img/roughness_length_fig2.png | Bin 0 -> 89916 bytes physics/docs/img/sice_wonton2000_fig1.png | Bin 142025 -> 0 bytes physics/docs/library.bib | 173 +++++++++++++++++- physics/docs/txt/mainpage.txt | 33 +++- physics/gscond.f | 8 +- physics/gwdc.f | 5 - physics/gwdps.f | 6 - physics/mfdeepcnv.f | 3 - physics/mfshalcnv.f | 3 - physics/moninedmf.f | 3 - physics/ozphys.f | 3 - physics/radlw_main.f | 4 - physics/rayleigh_damp.f | 21 ++- physics/sfc_diag.f | 1 - physics/sfc_diff.f | 93 +++++++++- physics/sfc_drv.f | 92 ++++++---- physics/sfc_nst.f | 4 - physics/sfc_sice.f | 6 +- physics/sfcsub.f | 14 ++ physics/sflx.f | 62 ++++++- 27 files changed, 448 insertions(+), 110 deletions(-) create mode 100644 physics/docs/img/GFS_sice_wonton2000_fig1.png create mode 100644 physics/docs/img/Noah_LA_interaction.png create mode 100644 physics/docs/img/land_dataset.png create mode 100644 physics/docs/img/roughness_length_fig1.png create mode 100644 physics/docs/img/roughness_length_fig2.png delete mode 100644 physics/docs/img/sice_wonton2000_fig1.png diff --git a/physics/GFS_calpreciptype.f90 b/physics/GFS_calpreciptype.f90 index 1f3da9afb..adbd21581 100644 --- a/physics/GFS_calpreciptype.f90 +++ b/physics/GFS_calpreciptype.f90 @@ -1,19 +1,14 @@ !> \file GFS_calpreciptype.F90 -!! This file contains the subroutine that calculates dominant precipitation type (calpreciptype) -!! and its post. It is adopted from post but was made into a column to used by GFS model. +!! This file contains the subroutine that calculates dominant precipitation type (calpreciptype), +!! which provides precipitation forcing for LSM. !>\defgroup CALPRECIPTYPE GFS Dominant Precipitation Type !!\brief This scheme contains the subroutine that calculates dominant -!! precipitation type and its post. It is adopted from post but was made -!! into a column to used by GFS model. +!! precipitation type and its post, which provides precipitation forcing +!! to LSM !! -!!\section diagram Calling Hierarchy Diagram -!! placeholder !!\section intraphysics Intraphysics Communication -!! This space is reserved for a description of how this scheme uses info -!! from other scheme types and/or how information calculated in this -!! scheme is used in other scheme types. - +! module GFS_calpreciptype contains ! \section arg_table_GFS_calpreciptype_init Argument Table @@ -23,7 +18,7 @@ end subroutine GFS_calpreciptype_init !>\defgroup gfs_calpreciptype GFS calpreciptype Main !!\ingroup CALPRECIPTYPE -!!\brief blah blah +!!\brief This subroutine calculates dominant precipitation type, which provides precipitation forcing for LSM. !> \section arg_table_GFS_calpreciptype_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------|------------------------------------------------------------|---------|------|---------|-----------|--------|----------| diff --git a/physics/GFS_surface_loop_control.f b/physics/GFS_surface_loop_control.f index da1d2b188..14ab97afc 100644 --- a/physics/GFS_surface_loop_control.f +++ b/physics/GFS_surface_loop_control.f @@ -4,7 +4,6 @@ !> \defgroup GFS_surface_loop_control GFS_surface_loop_control scheme !! @{ !! \brief Brief description of the parameterization -!! \section diagram Calling Hierarchy Diagram !! \section intraphysics Intraphysics Communication module GFS_surface_loop_control_part1 @@ -57,7 +56,6 @@ end module GFS_surface_loop_control_part1 !> \defgroup GFS_surface_loop_control GFS_surface_loop_control scheme !! @{ !! \brief Brief description of the parameterization -!! \section diagram Calling Hierarchy Diagram !! \section intraphysics Intraphysics Communication module GFS_surface_loop_control_part2 diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index 4b5a08bfe..341095c55 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -126,7 +126,10 @@ INPUT = txt/mainpage.txt \ ### Land Surface ../sfc_drv.f \ ../sflx.f \ + ../sfcsub.f \ ../sfc_diff.f \ + 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using BibDesk. %% http://bibdesk.sourceforge.net/ -%% Created for Man Zhang at 2018-01-25 08:40:47 -0700 +%% Created for Man Zhang at 2018-01-31 17:02:44 -0700 %% Saved with string encoding Unicode (UTF-8) +@article{dorman_and_sellers_1989, + Author = {J. L. Dorman and P. J. Sellers}, + Date-Added = {2018-01-31 23:58:04 +0000}, + Date-Modified = {2018-02-01 00:02:39 +0000}, + Journal = {Journal of Applied Meteorology}, + Pages = {833-855}, + Title = {A global climatology of albedo, roughness length and stomatal resistance for atmospheric general circulation models as represented by the simple biosphere model (SiB)}, + Volume = {28}, + Year = {1989}} + +@misc{zobler_1999, + Author = {Oak Ridge National Laboratory Distributed Active Archive Center}, + Date-Added = {2018-01-31 23:52:28 +0000}, + Date-Modified = {2018-01-31 23:56:02 +0000}, + Howpublished = {Available on-line [http://www.daac.ornl.gov]}, + Month = {1999}, + Title = {Global soil types, 1-Degree Grid (Zobler). Dataset}} + +@techreport{zobler_1986, + Address = {New York, New York, USA}, + Author = {L. Zobler}, + Date-Added = {2018-01-31 23:47:42 +0000}, + Date-Modified = {2018-01-31 23:57:41 +0000}, + Institution = {NASA Goddard Institute for Space Studies}, + Number = {NASA Technical Memorandum 87802}, + Title = {A world soil file for global climate modelling}, + Year = {1986}} + +@article{hirsch_et_al_2015, + Author = {A. L. Hirsch and A.J. Pitman and J. Kala and R. Lorenz and M. G. Donat}, + Date-Added = {2018-01-31 23:30:18 +0000}, + Date-Modified = {2018-01-31 23:32:47 +0000}, + Journal = {Earth Interactions}, + Number = {12}, + Pages = {1-24}, + Title = {Modulation of land-use change impacts on temperature extremes via land-atmosphere coupling over Australia}, + Volume = {19}, + Year = {2015}} + +@article{findell_et_al_2017, + Author = {K. L. Findell and A. Berg and P. Gentine and J. P. Krasting and B. R. Lintner and S. Malyshev and J. A. Santanello and Jr. Shevliakova and E. Shevliakova}, + Date-Added = {2018-01-31 23:23:37 +0000}, + Date-Modified = {2018-01-31 23:27:28 +0000}, + Journal = {Nature Communications}, + Number = {989}, + Title = {The impact of anthropogenic land use and land cover change on regional climate extremes}, + Volume = {8}, + Year = {2017}} + +@article{koster_et_al_2014, + Author = {R. D. Koster and Y. Chang and S. D. Schubert}, + Date-Added = {2018-01-31 23:14:32 +0000}, + Date-Modified = {2018-01-31 23:18:15 +0000}, + Journal = {J. Climate}, + Pages = {9290-9301}, + Title = {A mechanism for land-atmosphere feedback involving planetary wave structures}, + Volume = {27}, + Year = {2014}} + +@article{hsu_et_al_2017, + Author = {H. Hsu and M.-H. Lo and B. P. Guillod and D. G. Miralles and S. Kumar}, + Date-Added = {2018-01-31 23:06:25 +0000}, + Date-Modified = {2018-01-31 23:12:23 +0000}, + Journal = {J. Geophys. Res. Atmos.}, + Pages = {6319-6328}, + Title = {Relation between precipitation location and antecedent/subsequent soil moisture spatial patterns}, + Volume = {122}, + Year = {2017}} + +@article{andersen_and_shepherd_2014, + Author = {T. K. Andersen and J. M. Shepherd}, + Date-Added = {2018-01-31 22:57:14 +0000}, + Date-Modified = {2018-01-31 23:04:07 +0000}, + Journal = {International Journal of Climatology}, + Pages = {391-402}, + Title = {A global spatiotemporal analysis of inland tropical cyclone maintenance or intensification}, + Volume = {34}, + Year = {2014}} + +@article{guillod_et_al_2015, + Author = {B.P. Guillod and B. Orlowsky and D. G. Miralles and A. J. Teuling and S. I. Seneviratne}, + Date-Added = {2018-01-31 22:46:31 +0000}, + Date-Modified = {2018-01-31 22:55:08 +0000}, + Journal = {Nature Communications}, + Number = {6443}, + Title = {Reconciling spatial and temporal soil moisture effects on afternoon rainfall}, + Volume = {6}, + Year = {2015}} + +@article{milovac_et_al_2016, + Author = {J. Milovac and K. Warrach-Sagi and A. Behrendt and F. Spath and J. Ingwersen and V. Wulfmeryer}, + Date-Added = {2018-01-31 22:35:04 +0000}, + Date-Modified = {2018-01-31 22:43:31 +0000}, + Journal = {J. Geophys. Res. Atmos.}, + Pages = {624-649}, + Title = {Investigation of PBL schemes combining the WRF model simulations with scanning waver vapor differential absorption lidar measurements}, + Volume = {121}, + Year = {2016}} + +@article{paimazumder_and_done_2016, + Author = {D. PaiMazumder and J. M. Done}, + Date-Added = {2018-01-31 22:30:34 +0000}, + Date-Modified = {2018-01-31 22:33:52 +0000}, + Journal = {J. Geophys. Res. Atmos.}, + Pages = {12581-12592}, + Title = {Potential predictability sources of the 2012 U.S. drought in observations and a regional model ensemble}, + Volume = {121}, + Year = {2016}} + +@article{betts_et_al_2017, + Author = {A. K. Betts and A. B. Tawfik and R. L. Desjardins}, + Date-Added = {2018-01-31 18:31:50 +0000}, + Date-Modified = {2018-01-31 18:35:17 +0000}, + Journal = {J. Hydrometeorol.}, + Number = {939-955}, + Title = {Revisiting hydrometeorology using cloud and climate observations}, + Volume = {18}, + Year = {2017}} + +@article{ek_and_holtslag_2004, + Author = {M. B. Ek and A. A. M. Holtslag}, + Date-Added = {2018-01-31 17:43:57 +0000}, + Date-Modified = {2018-01-31 17:47:18 +0000}, + Journal = {J. Hydrometeorol.}, + Pages = {86-99}, + Title = {Influence of soil moisture on boundary layer cloud development}, + Volume = {5}, + Year = {2004}} + +@article{ek_and_mahrt_1994, + Author = {M. Ek and L. Mahrt}, + Date-Added = {2018-01-31 17:41:59 +0000}, + Date-Modified = {2018-01-31 17:43:53 +0000}, + Journal = {Monthly Weather Review}, + Pages = {2709-2721}, + Title = {Daytime evolution of relative-humidity at the boundary-layer top}, + Volume = {122}, + Year = {1994}} + +@article{zheng_et_al_2012, + Author = {W. Zheng and H. Wei and Z. Wang and X. Zeng and J. Meng and M. Ek and K. Mitchell and J. Derber}, + Date-Added = {2018-01-29 23:48:13 +0000}, + Date-Modified = {2018-01-29 23:51:19 +0000}, + Journal = {J. Geophys. Res.}, + Number = {D06117}, + Title = {Improvement of daytime land surface skin temperature over arid regions in the NCEP GFS model and its impact on satellite data assimilation}, + Volume = {117}, + Year = {2012}} + +@article{zeng_and_dickinson_1998, + Author = {X. Zeng and R.E. Dickinson}, + Date-Added = {2018-01-29 23:46:03 +0000}, + Date-Modified = {2018-01-29 23:47:43 +0000}, + Journal = {J. Climate}, + Pages = {537-550}, + Title = {Effect of surface sublayer on surface skin temperature and fluxes}, + Volume = {11}, + Year = {1998}} + +@conference{zheng_et_al_2009, + Address = {Omaha, Nebraska}, + Author = {W. Zheng and H. Wei and J. Meng and M. Ek and K. Mitchell and J. Derber and X. Zeng and Z. Wang}, + Date-Added = {2018-01-26 22:19:06 +0000}, + Date-Modified = {2018-01-29 23:51:37 +0000}, + Organization = {The 23rd Conference on Weather Analysis and Forecasting (WAF)/19th Conference on Numerical Weather Prediction(NWP)}, + Title = {Improvement of land surface skin temperature in NCEP Operational NWP models and its impact on satellite Data Assimilation}, + Year = {2009}, + Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUGJCVYJHZlcnNpb25YJG9iamVjdHNZJGFyY2hpdmVyVCR0b3ASAAGGoKgHCBMUFRYaIVUkbnVsbNMJCgsMDxJXTlMua2V5c1pOUy5vYmplY3RzViRjbGFzc6INDoACgAOiEBGABIAFgAdccmVsYXRpdmVQYXRoWWFsaWFzRGF0YV8QXC4uLy4uLy4uLy4uLy4uLy4uLy4uL0Rlc2t0b3AvTk9BSF9MU00vSW1wcm92ZW1lbnRfb2ZfTGFuZF9TdXJmYWNlX1NraW5fVGVtcGVyYXR1cmVfaW5fTkMucGRm0hcLGBlXTlMuZGF0YU8RAiAAAAAAAiAAAgAADE1hY2ludG9zaCBIRAAAAAAAAAAAAAAAAAAAANPh2NdIKwAAA2XmtR9JbXByb3ZlbWVudF9vZl9MYW5kIzM2NUZGMEYucGRmAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAADZf8P1pDvzQAAAAAAAAAAAAcAAwAACSAAAAAAAAAAAAAAAAAAAAAITk9BSF9MU00AEAAIAADT4i03AAAAEQAIAADWkVI9AAAAAQAQA2XmtQAPxiAAD8YPAAYv3gACAFFNYWNpbnRvc2ggSEQ6VXNlcnM6AG1hbi56aGFuZzoARGVza3RvcDoATk9BSF9MU006AEltcHJvdmVtZW50X29mX0xhbmQjMzY1RkYwRi5wZGYAAA4AbgA2AEkAbQBwAHIAbwB2AGUAbQBlAG4AdABfAG8AZgBfAEwAYQBuAGQAXwBTAHUAcgBmAGEAYwBlAF8AUwBrAGkAbgBfAFQAZQBtAHAAZQByAGEAdAB1AHIAZQBfAGkAbgBfAE4AQwAuAHAAZABmAA8AGgAMAE0AYQBjAGkAbgB0AG8AcwBoACAASABEABIAV1VzZXJzL21hbi56aGFuZy9EZXNrdG9wL05PQUhfTFNNL0ltcHJvdmVtZW50X29mX0xhbmRfU3VyZmFjZV9Ta2luX1RlbXBlcmF0dXJlX2luX05DLnBkZgAAEwABLwAAFQACABD//wAAgAbSGxwdHlokY2xhc3NuYW1lWCRjbGFzc2VzXU5TTXV0YWJsZURhdGGjHR8gVk5TRGF0YVhOU09iamVjdNIbHCIjXE5TRGljdGlvbmFyeaIiIF8QD05TS2V5ZWRBcmNoaXZlctEmJ1Ryb290gAEACAARABoAIwAtADIANwBAAEYATQBVAGAAZwBqAGwAbgBxAHMAdQB3AIQAjgDtAPIA+gMeAyADJQMwAzkDRwNLA1IDWwNgA20DcAOCA4UDigAAAAAAAAIBAAAAAAAAACgAAAAAAAAAAAAAAAAAAAOM}} + @article{chen_et_al_1997, Author = {F. Chen and Z. Janjic and K. Mitchell}, Date-Added = {2018-01-25 03:23:50 +0000}, @@ -15,7 +184,7 @@ @article{chen_et_al_1997 Journal = {Boundary-Layer Meteorology}, Number = {3}, Pages = {391-421}, - Title = {Impact of atmospheric surface-layer parameterizations in the new land-surface scheme of the NCEP mesoscale Eta model }, + Title = {Impact of atmospheric surface-layer parameterizations in the new land-surface scheme of the NCEP mesoscale Eta model}, Volume = {85}, Year = {1997}} diff --git a/physics/docs/txt/mainpage.txt b/physics/docs/txt/mainpage.txt index 30ba3eb56..93e99b9b2 100644 --- a/physics/docs/txt/mainpage.txt +++ b/physics/docs/txt/mainpage.txt @@ -1,17 +1,46 @@ /** \mainpage 2017 GFS Operational Physics -The documentation found here corresponds to the state of the operational GFS physics suite as of 2017. Documentation for the operational physics suite can be access through these links:: +\section updates 2017 GFS Physics Upgrades +Effective on Wednesday July 19, 2017, beginning with the 1200 UTC run, NCEP has upgraded the GFS physics as follows: + - Implement Near Surface Sea Temperature (NSST) to replace Real-Time Global SST (RTGSST) to provide more realistic ocean boundary conditions + - Changes to cumulus convection + - Scale-aware, aerosol-aware + - Rain conversion rate decreases with decreasing air temperature above freezing level + - Convective adjustment time in deep convection proportional to convective turn-over time with CAPE approaching zero after adjustment time + - Cloud base mass flux in shallow convection as a function of mean updraft velocity + - Convection trigger condition to suppress the unrealistic summertime spotty precipitation over high mountains + - Convective cloudiness enhanced by suspended cloud condensate in updraft + - A 50% reduction in Rayleigh damping in the upper stratosphere above 2 hPa that improves stratospheric fields + - Land surface changes: + - IGBP 20-type 1-km land classification + - STASGO 19-type 1-km soil classification + - MODIS-based snow free albedo + - MODIS-based maximum snow albedo + - Diurnal albedo treatment + - Unify snow cover, albedo between radiation and land surface model + - Increase ground heat flux under deep snow + - Upgrade surface layer parameterization scheme to modify the roughness-length formulation and introduce a stability parameter constraint in the Monin-Obukhov similarity theory to prevent the land-atmosphere system from fully decoupling leading to excessive cooling of 2m temperature during sunset + +Changes in the land surface and stability parameter should reduce a near surface wintertime cold bias, a rapid temperature drop during sunset and reduce a blockiness apparent in some near-surface fields. Some nighttime warm biases were introduced. Changes in convection should reduce a positive bias in light amounts of precipitation and unrealistic summertime spotty precipitation over high mountains and increase skill in forecasting precipitation. NSST is expected to improve tropical forecasts and may affect mid-latitude oceanic storms. Reducing Rayleigh damping improved wind and temperature forecast in the upper stratosphere. + +Details on the changes and evaluation of the changes of the entire Global Forecast System can be found at: +\n http://www.emc.ncep.noaa.gov/gmb/noor/GFS2017/GFS2017.htm + +\section schemes CCPP Physics Documentation +The documentation found here corresponds to the state of the operational GFS physics suite as of 2017. Documentation for the operational physics suite can be access through these links: - \ref RRTMG - \ref SAMF - \ref SAMF_shal - \ref HEDMF - \ref Zhao-Carr - - \ref NOAH - \ref Sfc_ex_cal - \ref GFS_Ice + - \ref NOAH - \ref GFS_NSST - \ref GFS_ogwd + - \ref GFS_rayleigh - \ref GFS_cgwd - \ref GFS_ozn + - \ref CALPRECIPTYPE */ diff --git a/physics/gscond.f b/physics/gscond.f index 5ae090b7c..98e87e1f4 100644 --- a/physics/gscond.f +++ b/physics/gscond.f @@ -36,14 +36,8 @@ module GFS_zhaocarr_gscond !! conversion from condensate (water and ice) to precipitation !! - EVPCO: Coefficient for evaporation of precipitation !! -!! \section diagram Calling Hierarchy Diagram -!! -!! \todo zhao-carr calling hierarchy diagram -!! !! \section intraphysics Intraphysics Communication -!! \todo zhao-carr intraphysics communication - - +!! !> \defgroup condense Grid-Scale Condensation and Evaporation of Cloud !! @{ diff --git a/physics/gwdc.f b/physics/gwdc.f index 21b80bba2..df12134d5 100644 --- a/physics/gwdc.f +++ b/physics/gwdc.f @@ -61,12 +61,7 @@ !! positive effects from using the parameterization are seen in the !! tropical upper troposphere and lower stratosphere. !! -!> \section diagram Calling Hierarchy Diagram -!! -!! \todo gwdc calling hierarchy diagram -!! !> \section intraphysics Intraphysics Communication -!! \todo gwdc calling hierarchy diagram module gwdc_pre contains diff --git a/physics/gwdps.f b/physics/gwdps.f index 7165c697e..e5c8838ff 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -95,13 +95,7 @@ !! four times stronger mountain blocking and one half the strength of !! gravity wave drag than the T383L64 version. !! -!> \section diagram Calling Hierarchy Diagram -!! -!! \todo gwdps calling hierarchy diagram -!! !> \section intraphysics Intraphysics Communication -!! \todo gwdps interaphysics communication - module gwdps_pre diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 00db6808e..ca6c85bc9 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -52,10 +52,7 @@ !! cloud condensate in the updraft. The lateral entrainment is also enhanced !! to more strongly suppress convection in a drier environment. !! -!! \section diagram Calling Hierarchy Diagram -!! \todo mfdeepcnv calling hierarchy diagram !! \section intraphysics Intraphysics Communication -!! \todo mfshalcnv intraphysics diagram !! This space is reserved for a description of how this scheme uses information !! from other scheme types and/or how information calculated in this scheme !! is used in other scheme types. diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 2ac467113..9dbabb4e6 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -22,10 +22,7 @@ !! \cite han_et_al_2017 . Details of scale- and aerosol-aware parameterizations !! are described in Han et al. (2017) \cite han_et_al_2017 . !! -!! \section diagram Calling Hierarchy Diagram -!! \todo mfshalcnv calling hierarchy diagram !! \section intraphysics Intraphysics Communication -!! \todo mfshalcnv intraphysics communitcation module sasas_shal contains diff --git a/physics/moninedmf.f b/physics/moninedmf.f index ec0fb4bb0..779cffd11 100644 --- a/physics/moninedmf.f +++ b/physics/moninedmf.f @@ -12,10 +12,7 @@ module edmf !! !! The PBL scheme's main task is to calculate tendencies of temperature, moisture, and momentum due to vertical diffusion throughout the column (not just the PBL). The scheme is an amalgamation of decades of work, starting from the initial first-order PBL scheme of Troen and Mahrt (1986) \cite troen_and_mahrt_1986, implemented according to Hong and Pan (1996) \cite hong_and_pan_1996 and modified by Han and Pan (2011) \cite han_and_pan_2011 and Han et al. (2015) \cite han_et_al_2015 to include top-down mixing due to stratocumulus layers from Lock et al. (2000) \cite lock_et_al_2000 and replacement of counter-gradient terms with a mass flux scheme according to Siebesma et al. (2007) \cite siebesma_et_al_2007 and Soares et al. (2004) \cite soares_et_al_2004. Recently, heating due to TKE dissipation was also added according to Han et al. (2015) \cite han_et_al_2015. !! -!! \section diagram Calling Hierarchy Diagram -!! \todo pbl calling hierarchy diagram !! \section intraphysics Intraphysics Communication -!! \todo pbl intraphysics communication subroutine edmf_init () end subroutine edmf_init diff --git a/physics/ozphys.f b/physics/ozphys.f index 5c5d101f8..743678066 100644 --- a/physics/ozphys.f +++ b/physics/ozphys.f @@ -12,10 +12,7 @@ !! Original version of these terms were provided by NASA/DAO based on !! NASA 2D Chemistry model - GSM is capable of running both versions !! -!! \section diagram Calling Hierarchy Diagram -!! \todo ozphys calling hierarchy diagram !! \section intra_oz Intraphysics Communication -!! \todo ozphys intraphysics communication !! module ozphys_pre contains diff --git a/physics/radlw_main.f b/physics/radlw_main.f index 8cb1d7a68..69bf5d83f 100644 --- a/physics/radlw_main.f +++ b/physics/radlw_main.f @@ -91,11 +91,7 @@ !! degree horizontal resolution is used, while a global mean monthly !! value is used in the upper atmosphere. !! -!> \section diagram Calling Hierarchy Diagram -!! \todo RRTMG calling hierarchy diagram -!! !> \section intraphysics Intraphysics Communication -!! \todo RRTMG intraphysics communication ! !!!!! ============================================================== !!!!! diff --git a/physics/rayleigh_damp.f b/physics/rayleigh_damp.f index a271f940a..c8d12c705 100644 --- a/physics/rayleigh_damp.f +++ b/physics/rayleigh_damp.f @@ -1,12 +1,27 @@ +!>\file rayleigh_damp.f +!! This file contains the Rayleigh friction calculation with total +!! energy conservation. module rayleigh_damp contains - -!! \section arg_table_rayleigh_damp_init Argument Table -!! +!>\defgroup GFS_rayleigh GFS Rayleigh Damping Calculation +!! \brief This is the Rayleigh friction calculation with total energy conservation. +!! Role of Rayleigh friction, it attempts to resolve two issues: +!! - The top lid model effects, sponge layer to suppress resolved wave reflections and extra-heating +!! - The winter-summer zonal wind drag in the strato-mesosphere +! \section arg_table_rayleigh_damp_init Argument Table +! subroutine rayleigh_damp_init () end subroutine rayleigh_damp_init +!>\defgroup rayleigh_main Rayleigh Damping Main +!!\ingroup GFS_rayleigh +!!\brief This is the Rayleigh friction calculation with total energy conservation. +!! Role of Rayleigh friction, it attempts to resolve two issues: +!! - The top lid model effects, sponge layer to suppress resolved wave reflections and extra-heating +!! - The winter-summer zonal wind drag in the strato-mesosphere +!! +!! !! \section arg_table_rayleigh_damp_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------|------------------------------------------------------|------------|------|---------|-----------|--------|----------| diff --git a/physics/sfc_diag.f b/physics/sfc_diag.f index 76517de2f..eb6a710fc 100644 --- a/physics/sfc_diag.f +++ b/physics/sfc_diag.f @@ -4,7 +4,6 @@ !> \defgroup Sfc_diag Land Surface Diagnose Calculation !! @{ !! \brief Brief description of the parameterization -!! \section diagram Calling Hierarchy Diagram !! \section intraphysics Intraphysics Communication module surface_diagnose diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index 6b991ab6c..e2d3d3ea6 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -1,13 +1,87 @@ !> \file sfc_diff.f -!! This file contains the surface exchange coefficient calculation scheme. +!! This file contains the surface roughness length formulation based on +!! the surface sublayer scheme from Zeng and Dickinson (1998) \cite +!! zeng_and_dickinson_1998. It is +!! the first subroutine called in surface layer loop. -!> \defgroup Sfc_ex_cal GFS Surface Exchange Coefficient Calculation +!> \defgroup Sfc_ex_cal GFS Surface Roughness Length Calculation !! @{ -!! \brief This is the first subroutine called in surface layer loop to calculate surface exchange ciefficients and near-surface wind. -!! \section diagram Calling Hierarchy Diagram -!! \todo sfc_diff Calling hierarchy diagram +!! \brief It is the surface roughness length formulation based on +!! the surface sublayer scheme from Zeng and Dickinson (1998) \cite +!! zeng_and_dickinson_1998. +!! +!! NOAH LSM are largely responsible for the quality +!! of model forecasts produced for near-surface weather parameters, such +!! as 2-meter air temperature (\a T2m) and surface skin temperature +!! (\a LST). LST is derived from the surface energy budget, and is +!! particularly important to remote sensing and data assimilation. How +!! precise these two parameters can be simulated by the model strongly +!! dependes on how accurate the surface heat fluxes are parameterized, +!! particularly the surface sensible heat flux (\a SH). The surface +!! thermal roughness length is a key parameter to determine \a SH. +!! Previous GFS version do not distinguish between the roughness length +!! for heat and momentum. The aerodynamic roughness \f$Z_{0m}\f$ is used +!! for wind, while the thermal roughness \f$Z_{0t}\f$ is used for heat and +!! water vapor. In general,\f$Z_{0m}\f$ is different from \f$Z_{0t}\f$, +!! because the transfer of momentum is affected by pressure fluctuations +!! in the turbulent waves behind the roughness elements, while for heat +!! and water vapor transfer no such dynamical mechanism exists. Zeng and +!! Dickinson (1998) \cite zeng_and_dickinson_1998 found that the surface +!! skin temperature can be at least 10 K higher when considering the surface +!! sublayer (or the variable ratio of the \f$Z_{0m}/Z_{0t}\f$ than without +!! in the desert summer afternoon. +!! +!! In May 2011, the new vegetation-dependent formulations of +!! momentum and thermal roughness formulation (Zheng et al. 2009 +!! \cite zheng_et_al_2009; Zheng et al. 2012 \cite zheng_et_al_2012 ) +!! was implemented to deal with the cold LST bias +!! over the arid western continental United States +!! (CONUS) during daytime. This LST bias contributes to large errors in +!! simulated satellite brightness temperatures over land by the Community +!! Radiative Transfer Model (CRTM) and hence the rejection of satellite +!! data in the NCEP Gridpoint Statistical Interpolation (GSI) system, +!! especially for surface-sensitive satellite channels. +!! +!! Zheng et al.(2009) \cite zhang_et_al_2009 proposed a new formulation on +!! \f$ln(Z_{0m}^,/Z_{0t})\f$ as follows: +!!\f[ +!! ln(Z_{0m}^,/Z_{0t})=(1-GVF)^2C_{zil}k(u*Z_{0g}/\nu)^{0.5} +!!\f] +!! where \f$Z_{0m}^,\f$ is the effective momentum roughness length +!! computed in the following equation for each grid, \f$Z_{0t}\f$ +!! is the roughness lenghth for heat, \f$C_{zil}\f$ is a coefficient +!! (taken as 0.8), k is the Von Karman constant (0.4), +!! \f$\nu=1.5\times10^{-5}m^{2}s^{-1}\f$ is the molecular viscosity, +!! \f$u*\f$ is the friction velocity, and \f$Z_{0g}\f$ is the bare +!! soil roughness length for momentum (taken as 0.01). +!! \n In order to consider the convergence of \f$Z_{0m}\f$ between +!! fully vegetated and bare soil, the effective \f$Z_{0m}^,\f$ is +!! computed: +!!\f[ +!! \ln(Z_{0m}^,)=(1-GVF)^{2}\ln(Z_{0g})+\left[1-(1-GVF)^{2}\right]\ln(Z_{0m}) +!!\f] +!! +!!\image html roughness_length_fig1.png "Figure 1: Comparison of LST simulated in GFS and verification with the observations. (a) Difference between GFS and GOES in the control run at 18:00 UTC; (b) Difference between GFS and GOES with the new formulation run at 18:00 UTC, averaged from 1 to 3 July 2007" width=10cm +!! +!! Figure 1 show the 3 day average land surface skin temperature predicted +!! by the GFS and comparison with the GOES-derived satellite measurements. +!! At 18:00 UTC (midday in local time over the central United States) in +!! the control run (Figure 1a), a substantial cold bias can be found over +!! the west half of CONUS (i.e., arid or semiarid regions). The new roughness +!! length formulations significantly reduce the cold bias in the western +!! CONUS, while the LST in the eastern CONUS, where the bias is small in +!! the control run, is not much affected +!! +!!\image html roughness_length_fig2.png "Fiure 2: Average diurnal cycle on 1-3 July 2007 for verification of LST with GOES (black) and SURFRAD (blue) at Desert Rock, Nevada; red and green lines are for the control and sensitivity runs, respectively" width=10cm +!! +!! The Desert Rock station (36.63^oN, 116.02^oW), located in the Nevada +!! desert,is one of the observation stations within the SURFRAD network. +!! The GOES-derived LST is very similar to the SURFRAD obervations (Figure 2). +!! However, the old GFS run produces very low LST, compared to the observations, +!! especially during daytime. During midday, the cold bias can reach up to +!! -15^oC. The new formulation run produces a reasonable LST diurnal cycle. +!! The daytime LST increases substantially and is very close to the observations. !! \section intraphysics Intraphysics Communication -!! \todo sfc_diff intraphysics communication module surface_exchange_coefficients contains @@ -22,7 +96,8 @@ end subroutine sfc_ex_coef_finalize !> \defgroup GFS_diff_main GFS sfc_diff Main !! \ingroup Sfc_ex_cal -!> \brief This is the first subroutine called in surface layer loop to calculate surface exchange coefficients and near-surface wind. +!> \brief This is the first subroutine called in surface layer loop to +!! calculate surface roughness length. !! \section arg_table_sfc_ex_coef_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|-------------------------------------------------|------------|------|---------|-----------|--------|----------| @@ -59,9 +134,9 @@ end subroutine sfc_ex_coef_finalize !!| redrag | flag_for_reduced_drag_coefficient_over_sea | flag for reduced drag coefficient over sea | flag | 0 | logical | | in | F | !! !! \section general General Algorithm -!! \todo sfc_ex_coef_run general algorithm +!! !! \section detailed Detailed Algorithm -!! \todo sfc_ex_coef_run Detailed Algorithm +!! !! @{ subroutine sfc_ex_coef_run & & (im,ps,u1,v1,t1,q1,z1, & diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index 5122150d8..4384462d7 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -2,42 +2,71 @@ !! This file contains the NOAH land surface scheme driver. !> \defgroup NOAH GFS NOAH Land Surface Scheme -!! \brief The Noah LSM(version 2.7) is the land model. +!! \brief This it the NOAH Land Surface Model (NOAH LSM). !! -!! In 2005, the NCEP Noah LSM (Version 2.7.1) replaced -!! the Oregon State University (OSU) LSM, which had been operational in the GFS since -!! the mid-1990s. The Noah LSM embodies about 10 years of upgrades (see Chen et.al. 1996 -!! \cite chen_et_al_1996; Koren et. al. 1999 \cite koren_et_al_1999; Ek et. al. 2003 -!! \cite ek_et_al_2003) to its ancestor, the OSU LSM. +!! Land-atmosphere interactions are a main driver of Earth's surface +!! water and energy budgets. The importance of the land surface is +!! rather intuitive, and has been demonstrated not only in terms of +!! predictability on daily to seasonal timescale (Betts et al. 2017 +!! \cite betts_et_al_2017), but also in terms +!! of influencing extremes such as drought and heatwaves (PaiMazumder and +!! Done, 2016 \cite paimazumder_and_done_2016), PBL evolution and cloud +!! formation (Milovac et al. 2016 \cite milovac_et_al_2016) and afternoon +!! convection (Guillod et al. 2015 \cite guillod_et_al_2015), and +!! tropical cyclone re-intensification (Andersen and Shepherd, 2014 \cite +!! andersen_and_shepherd_2014). Other linkages, such as the role of soil +!! moisture (SM) or vegetation heterogeneity in mesoscale circulation +!! (Hsu et al. 2017 \cite hsu_et_al_2017) and planetary waves (Koster +!! et al. 2014 \cite koster_et_al_2014), and those driven by land use +!! and land cover change or management (Hirsch et al. 2015 +!! \cite hirsch_et_al_2015, Findell et al. 2017 +!! \cite findell_et_al_2017) are topics of active research. !! -!! The Noah LSM upgrade includes an increase from two (10, 190 cm thick) to four -!! soil layers (10, 30, 60, 100 cm thick). addition of frozen soil physics, new -!! formulations for infiltration and runoff (giving more runoff for unsaturated -!! soils), revised physics of the snowpack and its influence on surface heat fluxes -!! and albedo, tuning and adding canopy resistance parameters, allowing spatially -!! varying root depth, revised treatment of ground heat flux and soil thermal -!! conductivity, reformulation of dependence of direct surface evaporation on first -!! layer soil moisture, and improved seasonality of green vegetation cover. The -!! frozen soil physics includes soil heat sinks/sources from freezing/thawing -!! and influences vertical transport of soil moisture, soil thermal conductivity -!! and heat capacity, and present prognostic states of snowpack water-equivalent (SWE), -!! total soil moisture (liquid plus frozen), soil temperature, canopy water, and skin -!! temperature. SWE divided by the snowpack depth gives the snowpack density. Total -!! soil moisture minus liquid soil moisture gives the frozen soil moisture. +!! Figure 1 is a schematic of local land-atmosphere interactions in a +!! quiescent synoptic regime, including the soil moisture-precipitation +!! (SM-P) feedback pathways. Solid arrows indicate a positive feedback +!! pathway, and large dashed arrows represent a negative feedback, while +!! red indicates radiative, black indicates surface layer and PBL, and +!! brown indicates land surface processes. Thin red and grey dashed lines +!! with arrows also represent positive feedbacks. The single horizontal +!! gay-dotted line (no arrows) indicates the top of the PBL, and the seven +!! small vertical dashed lines (no arrows) represent precipitation +!! \image html Noah_LA_interaction.png "Figure 1: Local Land-atmosphere Interaction (courtesy of Micheal Ek, Ek and Mahrt (1994),\cite ek_and_mahrt_1994, Ek and Holtslag (2004),\cite ek_and_holtslag_2004)" width=10cm +!! The land-surface model component was substantially upgraded from the Oregon +!! State University (OSU) land surface model to EMC's new NOAH Land Surface Model +!! (NOAH LSM) during the major implementation in the NCEP Global Forecast System +!! (GFS) on May 31, 2005. Forecast System (GFS). The NOAH LSM embodies about 10 +!! years of upgrades (see Chen et al. 1996 +!! \cite chen_et_al_1996; Koren et al. 1999 \cite koren_et_al_1999; Ek et al. 2003 +!! \cite ek_et_al_2003) to its ancestor, the OSU LSM. The NOAH LSM upgrade includes: +!! - An increase from two (10, 190 cm thick) to four soil layers (10, +!! 30, 60, 100 cm thick) +!! - Addition of frozen soil physics +!! - Add glacial ice treatment +!! - Two snowpack states (SWE, density) +!! - New formulations for infiltration and runoff account for sub-grid +!! variability in precipitation and soil moisture +!! - Revised physics of the snowpack and its influence on surface heat +!! fluxes and albedo +!! - Higher canopy resistance +!! - Spatially varying root depth +!! - Surface fluxes weighted by snow cover fraction +!! - Improved thermal conduction in soil/snow +!! - Improved seasonality of green vegetation cover. +!! - Improved evaporation treatment over bare soil and snowpack !! -!! To provide initial values of soil moisture/temperature, the Noah LSM land states -!! cycle continuous in the coupled atmosphere/land global model of the GDAS. These -!! land states respond to the global model's predicted land-surface forcing (precipitation, -!! surface radiation, near-surface air temperature, humidity, and wind speed). Since -!! the land component of the GDAS is forced by model prediction rather than observed -!! precipitation, we avoid undue drift by nudging soil moisture towards a monthly -!! global climatology(in GDAS only, not in forecast). +!! \image html land_dataset.png "Figure 2: Land Data Sets Used in NCEP Modeling Systems" width=10cm +!! +!! \section upgrads Land Surface Updrades in Q3FY17 GFS +!! - IGBP 20-type land classifications and STASGO 19 type soil classifications +!! - New MODIS-based snow free and max snow albedo +!! - Diurnal albedo treatment +!! - Unify snow cover and albedo between radiation driver and Noah LSM +!! - Fix excessive cooling of T2m during sunset +!! - Increase ground heat flux under the deep snow !! !! -!!\section diagram Calling Hierarchy Diagram -!! \todo NOAH calling hierarchy diagram !!\section Intraphysics Intraphysics Communication -!! \todo NOAH intraphysics communication !! ! \defgroup NOAH_pre NOAH Land Surface Pre ! \ingroup NOAH @@ -109,7 +138,6 @@ end module lsm_noah_pre ! \ingroup NOAH ! @{ ! \brief Brief description of the parameterization -! \section diagram Calling Hierarchy Diagram ! \section intraphysics Intraphysics Communication module lsm_noah_post @@ -356,9 +384,7 @@ end subroutine lsm_noah_finalize !!| wet1 | normalized_soil_wetness | normalized soil wetness | frac | 1 | real | kind_phys | out | F | !! !! \section general General Algorithm -!! \todo sfc_drv general algorithm !! \section detailed Detailed Algorithm -!! \todo sfc_drv detailed algorithm !! @{ subroutine lsm_noah_run & & ( im, km, ps, u1, v1, t1, q1, soiltyp, vegtype, sigmaf, & diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index bccd7d2b9..22fb4e554 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -118,7 +118,6 @@ end subroutine sfc_nst_finalize !! !! \section NSST_detailed_algorithm !! -!! \todo nsst detailed algorithm !! !> @{ subroutine sfc_nst_run & @@ -704,9 +703,6 @@ module sfc_nst_pre !! !! Blah blah blah description of parameterization !! -!! \section diagram Calling Hierarchy Diagram -!! -!! Blah blah blah diagram !! !! \section intraphysics Intraphysics Communication !! diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 74681977c..56a4ad02c 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -36,7 +36,7 @@ !! the surface temperature and ice temperature structure. In each model grid box, the heat and moisture !! fluxes and albedo are treated separately for the ice and the open water. !! -!!\image html sice_wonton2000_fig1.png "Fig.1 Schematic representation of the three-layer model" width=5cm +!!\image html GFS_sice_wonton2000_fig1.png "Fig.1 Schematic representation of the three-layer model" width=5cm !! The model has four prognostic variables: the snow layer thickness \f$h_s\f$, the ice layer thickness !! \f$h_i\f$, the upper and lower ice layer temperatures located at the midpoints of the layers !! \f$h_i/4\f$ and \f$3h_i/4\f$ below the ice surface, respectively \f$T_1\f$ and \f$T_2\f$. The temperature of @@ -46,9 +46,6 @@ !! The model consists of a zero-heat-capacity snow layer overlying two equally thick sea ice layers (Fig.1). !! The upper ice layer has a variable heat capacity to represent brine pockets. !! -!! -!! \section diagram Calling Hierarchy Diagram -!! !! \section intraphysics Intraphysics Communication !!\image html schematic_sice.png "Fig.2 NCEP Sea Ice Model System Diagram" width=10cm @@ -70,7 +67,6 @@ end subroutine sfc_sice_finalize !>\defgroup gfs_sice_main GFS sfc_sice Main -!> \todo gfs_sice_main brief blah blah !! @{ !! \ingroup GFS_Ice !! \section arg_table_sfc_sice_run Arguments diff --git a/physics/sfcsub.f b/physics/sfcsub.f index 2b854b761..9f4dd1b3d 100644 --- a/physics/sfcsub.f +++ b/physics/sfcsub.f @@ -1,3 +1,17 @@ +!>\file sfcsub.f +!! This file sets, updates and quility controls numerous surface fields +!! such as soil moisture and SST. +!! +!!\defgroup static Surface Static Fields +!!\ingroup NOAH +!!\brief The GFS physics module "sfcsub.f" sets, updates and quality +!! controls numerous surface fields such as soil moisture and SST. +!! +!! It is incorporated in the forcast model, CHGRES and CYCLE. One of its +!! important functions is to set several static fields (which only change +!! when the land/non-land mask changes) by interpolating global gaussian +!! fields (grib 1) to the model point. + module sfccyc_module implicit none save diff --git a/physics/sflx.f b/physics/sflx.f index 19b67ffd5..ecf725a39 100644 --- a/physics/sflx.f +++ b/physics/sflx.f @@ -1,7 +1,7 @@ !\file sflx.f -!! This file contains the NCEP Noah LSM (Version 2.7.1) +!! This file contains the NCEP NOAH LSM (Version 2.7.1) -!>\defgroup NOAH_LSM NCEP Noah LSM +!>\defgroup NOAH_LSM NCEP NOAH LSM !!\ingroup NOAH_drv !!\brief This is sub-driver for "NOAH/OSU LSM" family of physics subroutines. !! It is a soil/veg/snowpack land-surface model to update soil moisture, soil @@ -10,9 +10,7 @@ !! (excluding input atmospheric forcings of downward radiation and precip). !! !!\section general General Algorithm -!!\todo NOAH LSM general algorithm !!\section detailed Detailed Algorithm -!!\todo NOAH LSM detailed algorithm !! @{ !----------------------------------- subroutine sflx & @@ -2911,6 +2909,11 @@ end subroutine tdfcnd !----------------------------------- +!> This subroutine calculates soil moisture flux. The soil moisture +!! content (smc - a per unit volume measurement) is a dependent variable +!! that is updated with prognostic equations. The canopy moisture content +!! (cmc) is also updated. Frozen ground version: new states added: sh2o, +!! and frozen ground correction factor, frzfact and paramter slope. subroutine evapo & !................................... ! --- inputs: @@ -3057,6 +3060,9 @@ end subroutine evapo !----------------------------------- +!> This subroutine updates the temperature state of the soil column +!! based on the thermal diffusion equation and update the frozen soil +!! moisture content based on the temperature. subroutine shflx & !................................... ! --- inputs: @@ -3218,6 +3224,11 @@ end subroutine shflx !----------------------------------- +!> This subroutine calculates soil moisture flux. The soil moisture +!! content (smc - a per unit vulume measurement) is a dependent variable +!! that is updated with prognostic equations. The canopy moisture content +!! (cmc) is also updated. Frozen ground version: new states added: sh2o and +!! frozen ground correction factor, frzx and parameter slope. subroutine smflx & !................................... ! --- inputs: @@ -3424,6 +3435,11 @@ end subroutine smflx !----------------------------------- +!> This subroutine calculates compaction of a snowpack under conditions of +!! increasing snow density, as obtained from an approximate solution of +!! E. Anderson's differential equation (3.29),NOAA technical report NWS 19, +!! by Victor Koren, 03/25/95. subroutine will return new values of \a snowh +!! and \a sndens . subroutine snowpack & !................................... ! --- inputs: @@ -3586,6 +3602,7 @@ end subroutine snowpack !----------------------------------- +!> This subrtouine calculates direct soil evaporation. subroutine devap & !................................... ! --- inputs: @@ -3655,6 +3672,17 @@ end subroutine devap !----------------------------------- +!> This subroutine calculates amount of supercooled liquid soil water +!! content if temperature is below 273.15K (t0). It requires Newton-type +!! iteration to solve the nonlinear implicit equation given in eqn 17 +!! of Koren et al.(1999) \cite koren_et_al_1999. +!! +!! New version (June 2001): much faster and more accurate Newton iteration +!! achieved by first taking log of eqn cited above -- less than 4 (typically +!! 1 or 2) iterations achieves convergence. Also, explicit 1-step solution +!! option for special case of paramter ck=0, which reduces the orginal +!! implicit equation to a simpler explicit form, known as the "flerchinger eqn". +!! Improved handling of solution in the limit of freezing point temperature t0. subroutine frh2o & !................................... ! --- inputs: @@ -3806,6 +3834,10 @@ end subroutine frh2o !----------------------------------- +!> This subroutine calculates the right hand side of the time tendency +!! term of the soil thermal diffusion equation. Also to compute (prepare) +!! the matrix coefficients for the tri-diagonal matrix of the implicit time +!! scheme. subroutine hrt & !................................... ! --- inputs: @@ -4150,6 +4182,9 @@ end subroutine hrt !----------------------------------- +!> This subroutine calculates the right hand side of the time tendency +!! term of the soil thermal diffusion equation for sea-ice (ice = 1) or +!! glacial-ice (ice). subroutine hrtice & !................................... ! --- inputs: @@ -4322,6 +4357,7 @@ end subroutine hrtice !----------------------------------- +!> This subroutine calculates/updates the soil temperature field. subroutine hstep & !................................... ! --- inputs: @@ -4421,6 +4457,7 @@ end subroutine hstep !----------------------------------- +!> This subroutine inverts (solve) the tri-diagonal matrix problem. subroutine rosr12 & !................................... ! --- inputs: @@ -4523,6 +4560,7 @@ end subroutine rosr12 !----------------------------------- +!> This subroutine calculates sink/source term of the termal diffusion equation. subroutine snksrc & !................................... ! --- inputs: @@ -4664,6 +4702,10 @@ end subroutine snksrc !----------------------------------- +!> This subroutine calculates the right hand side of the time tendency +!! term of the soil water diffusion equation. Also to compute +!! (prepare) the matrix coefficients for the tri-diagonal matrix of +!! the implicit time scheme. subroutine srt & !................................... ! --- inputs: @@ -4974,6 +5016,8 @@ end subroutine srt !----------------------------------- +!> This subroutine calculates/updates soil moisture content values and +!! canopy moisture content values. subroutine sstep & !................................... ! --- inputs: @@ -5120,6 +5164,8 @@ end subroutine sstep !----------------------------------- +!> This subroutine calculates temperature on the boundary of the +!! layer by interpolation of the middle layer temperatures. subroutine tbnd & !................................... ! --- inputs: @@ -5190,6 +5236,11 @@ end subroutine tbnd !----------------------------------- +!> This subroutine calculates soil layer average temperature (tavg) +!! in freezing/thawing layer using up, down, and middle layer +!! temperature (tup, tdn, tm), where tup is at top boundary of layer, +!! tdn is at bottom boundary of layer. tm is layer prognostic state +!! temperature. subroutine tmpavg & !................................... ! --- inputs: @@ -5294,6 +5345,7 @@ end subroutine tmpavg !----------------------------------- +!> This subroutine calculates transpiration for the veg class. subroutine transp & !................................... ! --- inputs: @@ -5426,6 +5478,8 @@ end subroutine transp !----------------------------------- +!> This subroutine calculates soil water diffusivity and soil +!! hydraulic conductivity. subroutine wdfcnd & !................................... ! --- inputs: From a68f18b124bc2f4de1a66b828d390c955f15e7a0 Mon Sep 17 00:00:00 2001 From: "Man.Zhang" Date: Fri, 2 Feb 2018 16:58:28 -0700 Subject: [PATCH 08/22] fix some doxygen format warnings --- physics/GFS_calpreciptype.f90 | 6 ++--- physics/docs/ccpp_dox | 2 +- physics/gscond.f | 2 +- physics/mfdeepcnv.f | 5 +---- physics/mfpbl.f | 4 ++-- physics/mfshalcnv.f | 6 ++--- physics/moninedmf.f | 4 ++-- physics/ozphys.f | 2 +- physics/precpd.f | 2 +- physics/radiation_aerosols.f | 5 ++--- physics/radiation_astronomy.f | 2 -- physics/radiation_clouds.f | 6 ++--- physics/radiation_gases.f | 2 -- physics/radiation_surface.f | 2 +- physics/radlw_main.f | 8 ++----- physics/radlw_param.f | 2 -- physics/radsw_main.f | 4 +--- physics/radsw_param.f | 2 -- physics/sfc_diff.f | 16 ++++++------- physics/sfc_drv.f | 11 +++++---- physics/sfc_nst.f | 42 ++++++++++++++--------------------- physics/sfc_sice.f | 6 ++--- physics/sflx.f | 7 +++--- 23 files changed, 57 insertions(+), 91 deletions(-) diff --git a/physics/GFS_calpreciptype.f90 b/physics/GFS_calpreciptype.f90 index adbd21581..1566cb38d 100644 --- a/physics/GFS_calpreciptype.f90 +++ b/physics/GFS_calpreciptype.f90 @@ -1,4 +1,4 @@ -!> \file GFS_calpreciptype.F90 +!> \file GFS_calpreciptype.f90 !! This file contains the subroutine that calculates dominant precipitation type (calpreciptype), !! which provides precipitation forcing for LSM. @@ -50,9 +50,9 @@ end subroutine GFS_calpreciptype_init !! | srflag | flag_for_precipitation_type | snow(1)/rain(0) flag for precipitation | flag | 1 | real | kind_phys | out | F | !! | tprcp | nonnegative_lwe_thickness_of_precipitation_amount_on_dynamics_timestep | nonnegative precipitation amount in one dynamics time step | m | 1 | real | kind_phys | out | F | !! -!! \section general General Algorithm +!! \section general_calpreciptype General Algorithm !! -!! \section detailed Detailed Algorithm +!! \section detailed_calpreciptype Detailed Algorithm !! @{ subroutine GFS_calpreciptype_run(kdt,nrcm,im,ix,lm,lp1,randomno, & cal_pre, & diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index 341095c55..171044278 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -129,7 +129,7 @@ INPUT = txt/mainpage.txt \ ../sfcsub.f \ ../sfc_diff.f \ ../set_soilveg.f \ - ../GFS_calpreciptype.F90 \ + ../GFS_calpreciptype.f90 \ ### Sea Ice Surface ../sfc_sice.f \ ### Ocean Surface diff --git a/physics/gscond.f b/physics/gscond.f index 98e87e1f4..1e5013d07 100644 --- a/physics/gscond.f +++ b/physics/gscond.f @@ -36,7 +36,7 @@ module GFS_zhaocarr_gscond !! conversion from condensate (water and ice) to precipitation !! - EVPCO: Coefficient for evaporation of precipitation !! -!! \section intraphysics Intraphysics Communication +!! \section intraphysics_gscond Intraphysics Communication !! !> \defgroup condense Grid-Scale Condensation and Evaporation of Cloud !! @{ diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index ca6c85bc9..abaac1c9f 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -1,7 +1,6 @@ !> \file mfdeepcnv.f !! This file contains the entire SAMF deep convection scheme. !> \defgroup SAMF GFS Scale-Aware Mass-Flux Deep Convection -!! @{ !> \brief The scale-aware mass-flux (SAMF) deep convection scheme is an !! updated version of the previous Simplified Arakawa-Schubert (SAS) scheme !! with scale and aerosol awareness and parameterizes the effect of deep @@ -139,7 +138,7 @@ end subroutine sasasdeep_finalize !! | cnvw | convective_cloud_water_specific_humidity | convective cloud water | kg kg-1 | 2 | real | kind_phys | out | F | !! | cnvc | convective_cloud_cover | convective cloud cover | frac | 2 | real | kind_phys | out | F | !! -!! \section general General Algorithm +!! \section general_mfdeep General Algorithm !! -# Compute preliminary quantities needed for static, dynamic, and !! feedback control portions of the algorithm. !! -# Perform calculations related to the updraft of the entraining/detraining @@ -2669,6 +2668,4 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & return end subroutine sasasdeep_run !! @} -!! @} - end module sasas_deep diff --git a/physics/mfpbl.f b/physics/mfpbl.f index b368078b9..b36b98130 100644 --- a/physics/mfpbl.f +++ b/physics/mfpbl.f @@ -29,11 +29,11 @@ !! \param[in,out] ucko updraft u component of horizontal momentum (\f$ m s^{-1} \f$) !! \param[in,out] vcko updraft v component of horizontal momentum (\f$ m s^{-1} \f$) !! -!! \section general General Algorithm +!! \section general_mfpbl General Algorithm !! -# Determine an updraft parcel's entrainment rate, buoyancy, and vertical velocity. !! -# Recalculate the PBL height (previously calculated in moninedmf) and the parcel's entrainment rate. !! -# Calculate the mass flux profile and updraft properties. -!! \section detailed Detailed Algorithm +!! \section detailed_mfpbl Detailed Algorithm !! @{ subroutine mfpbl(im,ix,km,ntrac,delt,cnvflg, & & zl,zm,thvx,q1,t1,u1,v1,hpbl,kpbl, & diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 9dbabb4e6..6cbbada3b 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -1,7 +1,6 @@ !> \file mfshalcnv.f !! This file contains the entire SAMF deep convection scheme. !> \defgroup SAMF_shal GFS Scale-Aware Mass-Flux Shallow Convection -!! @{ !! \brief The scale-aware mass-flux shallow (SAMF_shal) convection !! scheme is an updated version of the previous mass-flux shallow !! convection scheme with scale and aerosol awareness and @@ -75,7 +74,7 @@ end subroutine sasasshal_init !! | cnvw | convective_cloud_water_specific_humidity | convective cloud water specific humidity | kg kg-1 | 2 | real | kind_phys | out | F | !! | cnvc | convective_cloud_cover | convective cloud cover | frac | 2 | real | kind_phys | out | F | !! -!! \section general General Algorithm +!! \section general_mfshal General Algorithm !! -# Compute preliminary quantities needed for the static and feedback !! control portions of the algorithm. !! -# Perform calculations related to the updraft of the entraining/detraining @@ -87,7 +86,7 @@ end subroutine sasasshal_init !! -# For the "feedback control", calculate updated values of the state !! variables by multiplying the cloud base mass flux and the tendencies !! calculated per unit cloud base mass flux from the static control. -!! \section detailed Detailed Algorithm +!! \section detailed_mfshal Detailed Algorithm !! @{ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & & ql2,q1,t1,u1,v1,rn,kbot,ktop,kcnv,islimsk,garea, & @@ -1708,7 +1707,6 @@ end subroutine sasasshal_run ! subroutine sasasshal_finalize end subroutine sasasshal_finalize -!! @} end module sasas_shal diff --git a/physics/moninedmf.f b/physics/moninedmf.f index 779cffd11..784c62af0 100644 --- a/physics/moninedmf.f +++ b/physics/moninedmf.f @@ -80,7 +80,7 @@ end subroutine edmf_finalize !! | lprnt | flag_print | flag for printing diagnostics to output | flag | 0 | logical | | in | F | !! | ipr | horizontal_index_of_printed_column | horizontal index of printed column | index | 0 | integer | | in | F | !! -!! \section general General Algorithm +!! \section general_edmf General Algorithm !! -# Compute preliminary variables from input arguments. !! -# Calculate the first estimate of the PBL height ("Predictor step"). !! -# Calculate Monin-Obukhov similarity parameters. @@ -94,7 +94,7 @@ end subroutine edmf_finalize !! -# Solve for the temperature and moisture tendencies due to vertical mixing. !! -# Calculate heating due to TKE dissipation and add to the tendency for temperature. !! -# Solve for the horizontal momentum tendencies and add them to output tendency terms. -!! \section detailed Detailed Algorithm +!! \section detailed_edmf Detailed Algorithm !! @{ subroutine edmf_run (ix,im,km,ntrac,ntcw,dv,du,tau,rtg, & & u1,v1,t1,q1,swh,hlw,xmu, & diff --git a/physics/ozphys.f b/physics/ozphys.f index 743678066..07188b53b 100644 --- a/physics/ozphys.f +++ b/physics/ozphys.f @@ -72,7 +72,7 @@ end subroutine ozphys_init !! | ozp | change_in_ozone_concentration | change in ozone concentration | kg kg-1 | 3 | real | kind_phys | inout | F | !! | me | mpi_rank | rank of the current MPI task | index | 0 | integer | default | in | F | !! -!! \section gen_al General Algorithm +!! \section genal_ozphys General Algorithm !> @{ subroutine ozphys_run ( & & ix, im, levs, ko3, dt, ozi, ozo, tin, po3, & diff --git a/physics/precpd.f b/physics/precpd.f index dd21c535d..2e7d090b2 100644 --- a/physics/precpd.f +++ b/physics/precpd.f @@ -45,7 +45,7 @@ end subroutine precpd_init !! | lprnt | flag_print | flag for printing diagnostics to output | flag | 0 | logical | | in | F | !! | jpr | horizontal_index_of_printed_column | horizontal index of printed column | index | 0 | integer | | in | F | !! -!! \section general General Algorithm +!! \section general_precpd General Algorithm !! The parameterization of precipitation is required in order to remove !! water from the atmosphere and transport it to the ground. In the !! scheme discussed here, simplifications in the precipitation diff --git a/physics/radiation_aerosols.f b/physics/radiation_aerosols.f index cf3dfbb52..6906699b8 100644 --- a/physics/radiation_aerosols.f +++ b/physics/radiation_aerosols.f @@ -117,7 +117,6 @@ !> \ingroup RRTMG !! \defgroup module_radiation_aerosols RRTMG Aerosols Module -!> @{ !! This module contains climatological atmospheric aerosol schemes for !! radiation computations. !! @@ -924,6 +923,7 @@ end subroutine wrt_aerlog !! solar spectral distribution, and define the one wavenumber IR fluxes !! based on black-body emission distribution at a predefined temperature. !>\section gel_set_spec General Algorithm +!! @{ !-------------------------------- subroutine set_spectrum !................................ @@ -1014,7 +1014,7 @@ subroutine set_spectrum !................................ end subroutine set_spectrum !-------------------------------- - +!! @} !> The initialization program for stratospheric volcanic aerosols. !----------------------------- @@ -5494,4 +5494,3 @@ end subroutine setgocartaer !..........................................! end module module_radiation_aerosols ! !==========================================! -!> @} diff --git a/physics/radiation_astronomy.f b/physics/radiation_astronomy.f index 1fe155ea2..601d9a581 100644 --- a/physics/radiation_astronomy.f +++ b/physics/radiation_astronomy.f @@ -77,7 +77,6 @@ !> \ingroup RRTMG !! \defgroup module_radiation_astronomy RRTMG Astronomy Module -!! @{ !> This module sets up astronomical quantities for solar radiation !! calculations. !! \version NCEP-Radiation_astronomy v5.2 Jan 2013 @@ -1008,4 +1007,3 @@ end subroutine prtime !...........................................! end module module_radiation_astronomy ! !===========================================! -!> @} diff --git a/physics/radiation_clouds.f b/physics/radiation_clouds.f index 654e320ad..42ef3908e 100644 --- a/physics/radiation_clouds.f +++ b/physics/radiation_clouds.f @@ -147,8 +147,7 @@ !> \ingroup RRTMG !! \defgroup module_radiation_clouds RRTMG Clouds Module -!! @{ -!> This module computes cloud related quantities for radiation +!! This module computes cloud related quantities for radiation !! computations. !! !! Knowledge of cloud properties and their vertical structure is @@ -172,7 +171,7 @@ !! - gethml():get diagnostic hi, mid, low,total,BL clouds !! - rhtable():rh lookup table for diag cloud scheme !! -!> \section gen_al General Algorithm +!> \section gen_al_clouds General Algorithm !! @{ !! -# Cloud Liquid/Ice Water Path (LWP,IWP) !!\n We define the fraction of liquid and ice cloud as: @@ -3399,4 +3398,3 @@ end subroutine rhtable !........................................! end module module_radiation_clouds ! !========================================! -!> @} diff --git a/physics/radiation_gases.f b/physics/radiation_gases.f index 75b57fcf8..09aa50e82 100644 --- a/physics/radiation_gases.f +++ b/physics/radiation_gases.f @@ -106,7 +106,6 @@ !> \ingroup RRTMG !! \defgroup module_radiation_gases RRTMG Gases Module -!! @{ !> This module sets up ozone climatological profiles and other constant !! gas profiles, such as co2, ch4, n2o, o2, and those of cfc gases. All !! data are entered as mixing ratio by volume, except ozone which is @@ -1166,4 +1165,3 @@ end subroutine getozn !........................................! end module module_radiation_gases ! !========================================! -!> @} diff --git a/physics/radiation_surface.f b/physics/radiation_surface.f index 9b5107906..09780030d 100644 --- a/physics/radiation_surface.f +++ b/physics/radiation_surface.f @@ -634,7 +634,7 @@ end subroutine setalb !!\param hprif (IMAX), topographic standard deviation in m !!\param IMAX array horizontal dimension !!\param sfcemis (IMAX), surface emissivity -!!\section general General Algorithm +!!\section general_setemis General Algorithm !> @{ !----------------------------------- subroutine setemis & diff --git a/physics/radlw_main.f b/physics/radlw_main.f index 69bf5d83f..05dbdc071 100644 --- a/physics/radlw_main.f +++ b/physics/radlw_main.f @@ -3,7 +3,6 @@ !! code from AER. !>\defgroup RRTMG GFS RRTMG Shortwave/Longwave Radiation Scheme -!! @{ !! \brief The GFS radiation scheme !! \details Radiative processes are among the most complex and !! computationally intensive parts of all model physics. As an @@ -38,8 +37,8 @@ !! \cite clough_et_al_1992) to compute absorption by water vapor at the !! continuum band. Longwave cloud radiative properties external to the !! RRTM depend on cloud liquid/ice water path and the effective radius -!! of ice particles and water droplets (Hu and Stamnes 1993 \cite -!! hu_and_stamnes_1993; Ebert and Curry 1992 \cite ebert_and_curry_1992). +!! of ice particles and water droplets (Hu and Stamnes 1993 +!! \cite hu_and_stamnes_1993; Ebert and Curry 1992 \cite ebert_and_curry_1992). !! !! Changes to Radiation Parameterization since 2007: !! \n The longwave (LW) and the shortwave (SW) radiation @@ -359,7 +358,6 @@ !! not sold and this copyright notice is reproduced on each copy made. !! This model is provided as is without any express or implied warranties. !! (http://www.rtweb.aer.com/) -!! @{ !========================================! module module_radlw_main ! !........................................! @@ -6754,5 +6752,3 @@ end subroutine taumol end module module_radlw_main ! !========================================! -!! @} -!! @} diff --git a/physics/radlw_param.f b/physics/radlw_param.f index 07d081271..b25dce356 100644 --- a/physics/radlw_param.f +++ b/physics/radlw_param.f @@ -3,7 +3,6 @@ !> \defgroup radlw_param GFS RADLW param Module !!\ingroup RRTMG -!! @{ !!!!! ============================================================== !!!!! !!!!! lw-rrtm3 radiation package description !!!!! @@ -161,4 +160,3 @@ module module_radlw_parameters ! !........................................! end module module_radlw_parameters ! !========================================! -!! @} diff --git a/physics/radsw_main.f b/physics/radsw_main.f index af512d47a..66e617635 100644 --- a/physics/radsw_main.f +++ b/physics/radsw_main.f @@ -399,7 +399,6 @@ !! not sold and this copyright notice is reproduced on each copy made. !! This model is provided as is without any express or implied warranties. !! (http://www.rtweb.aer.com/) -!! @{ !========================================! module module_radsw_main ! !........................................! @@ -3922,7 +3921,7 @@ end subroutine vrtqdr !!\param sfluxzen spectral distribution of incoming solar flux !!\param taug spectral optical depth for gases !!\param taur opt depth for rayleigh scattering -!>\section gen_al General Algorithm +!>\section gen_al_taumol General Algorithm !! @{ !----------------------------------- subroutine taumol & @@ -5410,4 +5409,3 @@ end subroutine taumol !........................................! end module module_radsw_main ! !========================================! -!! @} diff --git a/physics/radsw_param.f b/physics/radsw_param.f index d646fbf5e..48bad1715 100644 --- a/physics/radsw_param.f +++ b/physics/radsw_param.f @@ -3,7 +3,6 @@ !> \defgroup radsw_param GFS RADSW param Module !! \ingroup RRTMG -!! @{ !!!!! ============================================================== !!!!! !!!!! sw-rrtm3 radiation package description !!!!! @@ -200,4 +199,3 @@ module module_radsw_parameters ! !........................................! end module module_radsw_parameters ! !========================================! -!! @} diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index e2d3d3ea6..abeeaca27 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -1,14 +1,13 @@ !> \file sfc_diff.f !! This file contains the surface roughness length formulation based on -!! the surface sublayer scheme from Zeng and Dickinson (1998) \cite -!! zeng_and_dickinson_1998. It is +!! the surface sublayer scheme from Zeng and Dickinson (1998) +!! \cite zeng_and_dickinson_1998. It is !! the first subroutine called in surface layer loop. !> \defgroup Sfc_ex_cal GFS Surface Roughness Length Calculation -!! @{ !! \brief It is the surface roughness length formulation based on -!! the surface sublayer scheme from Zeng and Dickinson (1998) \cite -!! zeng_and_dickinson_1998. +!! the surface sublayer scheme from Zeng and Dickinson (1998) +!! \cite zeng_and_dickinson_1998. !! !! NOAH LSM are largely responsible for the quality !! of model forecasts produced for near-surface weather parameters, such @@ -42,7 +41,7 @@ !! data in the NCEP Gridpoint Statistical Interpolation (GSI) system, !! especially for surface-sensitive satellite channels. !! -!! Zheng et al.(2009) \cite zhang_et_al_2009 proposed a new formulation on +!! Zheng et al.(2009) \cite zheng_et_al_2009 proposed a new formulation on !! \f$ln(Z_{0m}^,/Z_{0t})\f$ as follows: !!\f[ !! ln(Z_{0m}^,/Z_{0t})=(1-GVF)^2C_{zil}k(u*Z_{0g}/\nu)^{0.5} @@ -133,9 +132,9 @@ end subroutine sfc_ex_coef_finalize !!| flag_iter | flag_for_iteration | flag for iteration | flag | 1 | logical | | in | F | !!| redrag | flag_for_reduced_drag_coefficient_over_sea | flag for reduced drag coefficient over sea | flag | 0 | logical | | in | F | !! -!! \section general General Algorithm +!! \section general_diff General Algorithm !! -!! \section detailed Detailed Algorithm +!! \section detailed_diff Detailed Algorithm !! !! @{ subroutine sfc_ex_coef_run & @@ -448,4 +447,3 @@ end subroutine sfc_ex_coef_run !! @} end module surface_exchange_coefficients -!! @} diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index 4384462d7..4b898588a 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -13,8 +13,8 @@ !! Done, 2016 \cite paimazumder_and_done_2016), PBL evolution and cloud !! formation (Milovac et al. 2016 \cite milovac_et_al_2016) and afternoon !! convection (Guillod et al. 2015 \cite guillod_et_al_2015), and -!! tropical cyclone re-intensification (Andersen and Shepherd, 2014 \cite -!! andersen_and_shepherd_2014). Other linkages, such as the role of soil +!! tropical cyclone re-intensification (Andersen and Shepherd, 2014 +!! \cite andersen_and_shepherd_2014). Other linkages, such as the role of soil !! moisture (SM) or vegetation heterogeneity in mesoscale circulation !! (Hsu et al. 2017 \cite hsu_et_al_2017) and planetary waves (Koster !! et al. 2014 \cite koster_et_al_2014), and those driven by land use @@ -31,7 +31,7 @@ !! with arrows also represent positive feedbacks. The single horizontal !! gay-dotted line (no arrows) indicates the top of the PBL, and the seven !! small vertical dashed lines (no arrows) represent precipitation -!! \image html Noah_LA_interaction.png "Figure 1: Local Land-atmosphere Interaction (courtesy of Micheal Ek, Ek and Mahrt (1994),\cite ek_and_mahrt_1994, Ek and Holtslag (2004),\cite ek_and_holtslag_2004)" width=10cm +!! \image html Noah_LA_interaction.png "Figure 1: Local Land-atmosphere Interaction (courtesy of Micheal Ek, Ek and Mahrt (1994), Ek and Holtslag (2004))" width=10cm !! The land-surface model component was substantially upgraded from the Oregon !! State University (OSU) land surface model to EMC's new NOAH Land Surface Model !! (NOAH LSM) during the major implementation in the NCEP Global Forecast System @@ -383,8 +383,8 @@ end subroutine lsm_noah_finalize !!| smcref2 | threshold_volume_fraction_of_condensed_water_in_soil | soil moisture threshold | frac | 1 | real | kind_phys | out | F | !!| wet1 | normalized_soil_wetness | normalized soil wetness | frac | 1 | real | kind_phys | out | F | !! -!! \section general General Algorithm -!! \section detailed Detailed Algorithm +!! \section general_noah General Algorithm +!! \section detailed_noah Detailed Algorithm !! @{ subroutine lsm_noah_run & & ( im, km, ps, u1, v1, t1, q1, soiltyp, vegtype, sigmaf, & @@ -830,4 +830,3 @@ end subroutine lsm_noah_run !! @} end module lsm_noah -!! @} diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index 22fb4e554..13450e793 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -23,7 +23,7 @@ !! \endhtmlonly !! @image html NSST.png "Figure 1: NSST profile." !! -!! \section intraphysics Intraphysics Communication +!! \section intraphysics_nst Intraphysics Communication !! !! This space is reserved for a description of how this scheme uses information from other scheme types and/or how information calculated in this scheme is used in other scheme types. @@ -698,7 +698,6 @@ module sfc_nst_pre contains ! \defgroup GFS_NSST_PRE GFS Near Sea Surface Temperature Pre -!! @{ !! \brief Brief description of the parameterization !! !! Blah blah blah description of parameterization @@ -743,11 +742,10 @@ end subroutine sfc_nst_pre_finalize !! | tsurf | surface_skin_temperature_after_iteration | ocean surface skin temperature for guess run | K | 1 | real | kind_phys | inout | F | !! | tskin | surface_skin_temperature | ocean surface skin temperature | K | 1 | real | kind_phys | out | F | !! -!! \section NSST_general_algorithm General Algorithm +! \section NSST_general_algorithm General Algorithm !! -!! Blah blah general algorithm !! -!! \section NSST_detailed_algorithm Detailed Algorithm +! \section NSST_detailed_algorithm Detailed Algorithm !! @{ subroutine sfc_nst_pre_run & & ( im, islimsk, oro, oro_uf, tsfc, tsurf, tskin ) @@ -783,8 +781,6 @@ subroutine sfc_nst_pre_run & return end subroutine sfc_nst_pre_run - -!> @} !! @} end module sfc_nst_pre @@ -796,7 +792,6 @@ module sfc_nst_post contains ! \defgroup GFS_NSST_POST GFS Near Sea Surface Temperature Post -!! @{ !! \brief Brief description of the parameterization !! !! Blah blah blah description of parameterization @@ -809,20 +804,19 @@ module sfc_nst_post !! !! Blah blah blah intraphysics communication -!> \brief Brief description of the subroutine -!! -!! Blah blah description of subroutine -!! -!! \section arg_table_sfc_nst_init Argument Table +! \brief Brief description of the subroutine +! +! Blah blah description of subroutine +! +! \section arg_table_sfc_nst_init Argument Table !! subroutine sfc_nst_post_init end subroutine sfc_nst_post_init -!> \brief Brief description of the subroutine +! \brief Brief description of the subroutine +! !! -!! Blah blah description of subroutine -!! -!! \section arg_table_sfc_nst_finalize Argument Table +! \section arg_table_sfc_nst_finalize Argument Table !! subroutine sfc_nst_post_finalize end subroutine sfc_nst_post_finalize @@ -852,12 +846,12 @@ end subroutine sfc_nst_post_finalize !! | dtzm | mean_change_over_depth_in_sea_water_temperature | mean of dT(z) (zsea1 to zsea2) | K | 1 | real | kind_phys | out | F | !! | tsfc | surface_skin_temperature | ocean surface skin temperature | K | 1 | real | kind_phys | out | F | !! -!! \section NSST_general_algorithm General Algorithm -!! -!! Blah blah general algorithm -!! -!! \section NSST_detailed_algorithm Detailed Algorithm -!! @{ +! \section NSST_general_algorithm General Algorithm +! +! Blah blah general algorithm +! +! \section NSST_detailed_algorithm Detailed Algorithm +! @{ subroutine sfc_nst_post_run & & ( im, islimsk, oro, oro_uf, nstf_name1, nstf_name4, & & nstf_name5, xt, xz, dt_cool, z_c, rslimsk, tref, xlon, & @@ -922,6 +916,4 @@ subroutine sfc_nst_post_run & return end subroutine sfc_nst_post_run -!! @} -!! @} end module sfc_nst_post diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 56a4ad02c..a0f13aa0a 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -46,7 +46,7 @@ !! The model consists of a zero-heat-capacity snow layer overlying two equally thick sea ice layers (Fig.1). !! The upper ice layer has a variable heat capacity to represent brine pockets. !! -!! \section intraphysics Intraphysics Communication +!! \section intraphysics_sice Intraphysics Communication !!\image html schematic_sice.png "Fig.2 NCEP Sea Ice Model System Diagram" width=10cm module sfc_sice @@ -113,8 +113,8 @@ end subroutine sfc_sice_finalize !! | evap | kinematic_surface_upward_latent_heat_flux | evaporative latent heat flux | kg kg-1 m s-1 | 1 | real | kind_phys | out | F | !! | hflx | kinematic_surface_upward_sensible_heat_flux | kinematic sensible heat flux | K m s-1 | 1 | real | kind_phys | out | F | !! -!! \section general General Algorithm -!! \section detailed Detailed Algorithm +!! \section general_sice_run General Algorithm +!! \section detailed_sice_run Detailed Algorithm !> @{ subroutine sfc_sice_run & & ( im, km, ps, u1, v1, t1, q1, delt, & diff --git a/physics/sflx.f b/physics/sflx.f index ecf725a39..e1b52a273 100644 --- a/physics/sflx.f +++ b/physics/sflx.f @@ -9,9 +9,8 @@ !! and all terms of the surface energy balance and surface water balance !! (excluding input atmospheric forcings of downward radiation and precip). !! -!!\section general General Algorithm -!!\section detailed Detailed Algorithm -!! @{ +!!\section general_sflx General Algorithm +!!\section detailed_sflx Detailed Algorithm !----------------------------------- subroutine sflx & !................................... @@ -5567,4 +5566,4 @@ end subroutine wdfcnd !................................... end subroutine sflx !----------------------------------- -!! @} + From dea06554ff10b0ad354eb18f5aaafa583f305eba Mon Sep 17 00:00:00 2001 From: "Man.Zhang" Date: Mon, 5 Feb 2018 11:57:31 -0700 Subject: [PATCH 09/22] more work on doxygen --- physics/docs/ccpp_dox | 1 + physics/docs/txt/mainpage.txt | 4 ++- physics/gwdc.f | 2 +- physics/gwdps.f | 2 +- physics/mfdeepcnv.f | 48 +++++++++++++++++------------------ physics/mfshalcnv.f | 38 ++++++++++++++------------- physics/moninedmf.f | 18 ++++++------- physics/sfc_diff.f | 6 ++--- physics/sfc_drv.f | 40 +++++++++++------------------ physics/sflx.f | 4 +-- physics/tridi.f | 12 ++++++++- 11 files changed, 91 insertions(+), 84 deletions(-) diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index 171044278..b2fd72275 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -120,6 +120,7 @@ INPUT = txt/mainpage.txt \ ### PBL ../moninedmf.f \ ../mfpbl.f \ + ../tridi.f \ ### Microphysics ../precpd.f \ ../gscond.f \ diff --git a/physics/docs/txt/mainpage.txt b/physics/docs/txt/mainpage.txt index 93e99b9b2..6fe8bb976 100644 --- a/physics/docs/txt/mainpage.txt +++ b/physics/docs/txt/mainpage.txt @@ -28,7 +28,8 @@ Details on the changes and evaluation of the changes of the entire Global Foreca \n http://www.emc.ncep.noaa.gov/gmb/noor/GFS2017/GFS2017.htm \section schemes CCPP Physics Documentation -The documentation found here corresponds to the state of the operational GFS physics suite as of 2017. Documentation for the operational physics suite can be access through these links: +Please check DTC website https://dtcenter.org/community-code/ipd-ccpp for GMTB IPD/CCPP infrastructure and governance information. +\n The documentation found here corresponds to the state of the operational GFS physics suite as of 2017. Documentation for the operational physics suite can be access through these links: - \ref RRTMG - \ref SAMF - \ref SAMF_shal @@ -43,4 +44,5 @@ The documentation found here corresponds to the state of the operational GFS phy - \ref GFS_cgwd - \ref GFS_ozn - \ref CALPRECIPTYPE + */ diff --git a/physics/gwdc.f b/physics/gwdc.f index df12134d5..4d0328368 100644 --- a/physics/gwdc.f +++ b/physics/gwdc.f @@ -52,7 +52,7 @@ !! the stable stratosphere can generate gravity waves that influence !! the large-scale flow. !! -!> \section provenance Provenance +!> \section provenance_gwdc Provenance !! - The parameterization of stationary convectively-forced GWD follows !! the development of Chun and Baik (1998) \cite chun_and_baik_1998 , !! which was tested in GCMs by Chun et al. (2001,2004) diff --git a/physics/gwdps.f b/physics/gwdps.f index e5c8838ff..69f146b63 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -56,7 +56,7 @@ !! seen as a source of gravity waves to the atmosphere above and !! nonlinear subgrid low-level mountain drag effect below. !! -!> \section provenance Provenance +!> \section provenance_gwdps Provenance !! - Gravity-wave drag is simulated as described by Alpert et al. !! (1988) \cite alpert_et_al_1988. The parameterization includes !! determination of the momentum flux due to gravity waves at the diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index abaac1c9f..5f83a29e7 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -59,28 +59,9 @@ module sasas_deep contains - -! \brief Brief description of the subroutine -! -! \section arg_table_sasasdeep_init Argument Table -! | local var name | longname | description | units | rank | type | kind | intent | optional | -! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| -! - subroutine sasasdeep_init - end subroutine sasasdeep_init - - -! \brief Brief description of the subroutine -! -! \section arg_table_sasasdeep_finalize Argument Table -! | local var name | longname | description | units | rank | type | kind | intent | optional | -! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| -! - subroutine sasasdeep_finalize - end subroutine sasasdeep_finalize - - !>\defgroup GFS_mfdeep GFS mfdeepcnv Main +!!\ingroup SAMF +!> @{ !>\brief This subroutine contains the entirety of the SAMF deep convection scheme. !! !! For grid sizes larger than threshold value, as in Grell (1993) @@ -101,11 +82,29 @@ end subroutine sasasdeep_finalize !! !! For grid sizes smaller than threshold value, the cloud base mass flux !! in the SAMF scheme is determined by the cumulus updraft velocity averaged -!! over the whole cloud depth (Han et al., 2017 \cite han_et_al_2017 ), which +!! over the whole cloud depth (Han et al., 2017 \cite han_et_al_2017 ),which !! in turn, determines changes of the large-scale environment due to the !! cumulus convection. !! -!! +! \brief Brief description of the subroutine +! +! \section arg_table_sasasdeep_init Argument Table +! | local var name | longname | description | units | rank | type | kind | intent | optional | +! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| +! + subroutine sasasdeep_init + end subroutine sasasdeep_init + + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasdeep_finalize Argument Table +! | local var name | longname | description | units | rank | type | kind | intent | optional | +! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| +! + subroutine sasasdeep_finalize + end subroutine sasasdeep_finalize + !! \section arg_table_sasasdeep_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------|-----------------------------------------------------|---------|------|---------|-----------|--------|----------| @@ -2666,6 +2665,7 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo !! return - end subroutine sasasdeep_run !! @} + end subroutine sasasdeep_run +!> @} end module sasas_deep diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 6cbbada3b..308602a0a 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -1,6 +1,11 @@ !> \file mfshalcnv.f !! This file contains the entire SAMF deep convection scheme. + + module sasas_shal + contains + !> \defgroup SAMF_shal GFS Scale-Aware Mass-Flux Shallow Convection +!> @{ !! \brief The scale-aware mass-flux shallow (SAMF_shal) convection !! scheme is an updated version of the previous mass-flux shallow !! convection scheme with scale and aerosol awareness and @@ -21,11 +26,8 @@ !! \cite han_et_al_2017 . Details of scale- and aerosol-aware parameterizations !! are described in Han et al. (2017) \cite han_et_al_2017 . !! -!! \section intraphysics Intraphysics Communication - - module sasas_shal - contains - +!! \section intraphysics_deep Intraphysics Communication +!! ! \brief Brief description of the subroutine ! ! \section arg_table_sasasshal_init Argument Table @@ -34,6 +36,7 @@ subroutine sasasshal_init end subroutine sasasshal_init !>\defgroup SAMF_shal_main GFS mfshalcnv Main +!!\ingroup SAMF_shal !> \brief The subroutine contains the entirety of the SAMF shallow convection scheme. !! This routine follows the \ref SAMF deep scheme quite closely, although !! it can be interpreted as only having the "static" and "feedback" control @@ -1698,8 +1701,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & enddo !! return - end subroutine sasasshal_run !! @} + end subroutine sasasshal_run ! \brief Brief description of the subroutine ! @@ -1708,15 +1711,16 @@ end subroutine sasasshal_run subroutine sasasshal_finalize end subroutine sasasshal_finalize +!> @} end module sasas_shal module sasas_shal_post contains -! \brief Brief description of the subroutine -! -! \section arg_table_sasasshal_post_run Argument Table -! | local var name | longname | description | units | rank | type | kind | intent | optional | +!! \brief Brief description of the subroutine +!! +!! \section arg_table_sasasshal_post_run Argument Table +!! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|----------------------------------------------------------|----------------------------------------------------------------------|---------|------|-------------------------------|-----------|--------|----------| !! | frain | dynamics_to_physics_timestep_ratio | ratio of dynamics timestep to physics timestep | none | 0 | real | kind_phys | in | F | !! | rain1 | lwe_thickness_of_shallow_convective_precipitation_amount | shallow convective rainfall amount on physics timestep | m | 1 | real | kind_phys | in | F | @@ -1766,17 +1770,17 @@ subroutine sasasshal_post_run (frain, rain1, cnvc, cnvw, Model, & end subroutine sasasshal_post_run -! \brief Brief description of the subroutine -! -! \section arg_table_sasasshal_post_init Argument Table +!! \brief Brief description of the subroutine +!! +!! \section arg_table_sasasshal_post_init Argument Table !! subroutine sasasshal_post_init () end subroutine sasasshal_post_init -! \brief Brief description of the subroutine -! -! \section arg_table_sasasshal_post_finalize Argument Table -! +!! \brief Brief description of the subroutine +!! +!! \section arg_table_sasasshal_post_finalize Argument Table +!! subroutine sasasshal_post_finalize () end subroutine sasasshal_post_finalize diff --git a/physics/moninedmf.f b/physics/moninedmf.f index 784c62af0..ca19993ed 100644 --- a/physics/moninedmf.f +++ b/physics/moninedmf.f @@ -1044,7 +1044,7 @@ subroutine edmf_run (ix,im,km,ntrac,ntcw,dv,du,tau,rtg, & ! ! solve tridiagonal problem for heat and moisture ! -!> The tridiagonal system is solved by calling the internal ::edmf_tridin subroutine. +!> The tridiagonal system is solved by calling tridin() subroutine. call tridin(im,km,ntrac,al,ad,au,a1,a2,au,a1,a2) ! @@ -1198,10 +1198,10 @@ end subroutine edmf_run !> @} c----------------------------------------------------------------------- -!> \ingroup HEDMF -!! \brief Routine to solve the tridiagonal system to calculate temperature and moisture at \f$ t + \Delta t \f$; part of two-part process to calculate time tendencies due to vertical diffusion. -!! -!! Origin of subroutine unknown. +! \ingroup HEDMF +! \brief Routine to solve the tridiagonal system to calculate temperature and moisture at \f$ t + \Delta t \f$; part of two-part process to calculate time tendencies due to vertical diffusion. +! +! Origin of subroutine unknown. C subroutine edmf_tridi2(l,n,cl,cm,cu,r1,r2,au,a1,a2) c C use machine , only : kind_phys @@ -1242,10 +1242,10 @@ end subroutine edmf_run C end C C----------------------------------------------------------------------- -!> \ingroup HEDMF -!! \brief Routine to solve the tridiagonal system to calculate u- and v-momentum at \f$ t + \Delta t \f$; part of two-part process to calculate time tendencies due to vertical diffusion. -!! -!! Origin of subroutine unknown. +! \ingroup HEDMF +! \brief Routine to solve the tridiagonal system to calculate u- and v-momentum at \f$ t + \Delta t \f$; part of two-part process to calculate time tendencies due to vertical diffusion. +! +! Origin of subroutine unknown. C subroutine edmf_tridin(l,n,nt,cl,cm,cu,r1,r2,au,a1,a2) c C use machine , only : kind_phys diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index abeeaca27..90e358d83 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -69,16 +69,16 @@ !! the west half of CONUS (i.e., arid or semiarid regions). The new roughness !! length formulations significantly reduce the cold bias in the western !! CONUS, while the LST in the eastern CONUS, where the bias is small in -!! the control run, is not much affected +!! the control run, is not much affected. !! !!\image html roughness_length_fig2.png "Fiure 2: Average diurnal cycle on 1-3 July 2007 for verification of LST with GOES (black) and SURFRAD (blue) at Desert Rock, Nevada; red and green lines are for the control and sensitivity runs, respectively" width=10cm !! -!! The Desert Rock station (36.63^oN, 116.02^oW), located in the Nevada +!! The Desert Rock station (\f$36.63^oN\f$, \f$116.02^oW\f$), located in the Nevada !! desert,is one of the observation stations within the SURFRAD network. !! The GOES-derived LST is very similar to the SURFRAD obervations (Figure 2). !! However, the old GFS run produces very low LST, compared to the observations, !! especially during daytime. During midday, the cold bias can reach up to -!! -15^oC. The new formulation run produces a reasonable LST diurnal cycle. +!! \f$-15^oC\f$. The new formulation run produces a reasonable LST diurnal cycle. !! The daytime LST increases substantially and is very close to the observations. !! \section intraphysics Intraphysics Communication diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index 4b898588a..b178585e5 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -57,21 +57,12 @@ !! !! \image html land_dataset.png "Figure 2: Land Data Sets Used in NCEP Modeling Systems" width=10cm !! -!! \section upgrads Land Surface Updrades in Q3FY17 GFS -!! - IGBP 20-type land classifications and STASGO 19 type soil classifications -!! - New MODIS-based snow free and max snow albedo -!! - Diurnal albedo treatment -!! - Unify snow cover and albedo between radiation driver and Noah LSM -!! - Fix excessive cooling of T2m during sunset -!! - Increase ground heat flux under the deep snow -!! -!! !!\section Intraphysics Intraphysics Communication !! -! \defgroup NOAH_pre NOAH Land Surface Pre -! \ingroup NOAH -! @{ -! \brief Brief description of the parameterization +!! \defgroup NOAH_pre NOAH Land Surface Pre +!! \ingroup NOAH +!! \brief Brief description of the parameterization +!! @{ module lsm_noah_pre contains @@ -82,9 +73,9 @@ end subroutine lsm_noah_pre_init subroutine lsm_noah_pre_finalize end subroutine lsm_noah_pre_finalize -! \brief Brief description of the subroutine -! -! \section arg_table_lsm_noah_pre_run Argument Table +!! \brief Brief description of the subroutine +!! +!! \section arg_table_lsm_noah_pre_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|--------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -129,17 +120,15 @@ subroutine lsm_noah_pre_run & end subroutine lsm_noah_pre_run -! @} end module lsm_noah_pre !! @} -! \defgroup NOAH_post NOAH Land Surface post -! \ingroup NOAH -! @{ -! \brief Brief description of the parameterization -! \section intraphysics Intraphysics Communication - +!! \defgroup NOAH_post NOAH Land Surface post +!! \ingroup NOAH +!! @{ +!! \brief Brief description of the parameterization +!! \section intraphysics Intraphysics Communication module lsm_noah_post contains @@ -149,8 +138,8 @@ end subroutine lsm_noah_post_init subroutine lsm_noah_post_finalize end subroutine lsm_noah_post_finalize -! \brief Brief description of the subroutine -! +!! \brief Brief description of the subroutine +!! !! \section arg_table_lsm_noah_post_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|--------------------------------------------|------------|------|---------|-----------|--------|----------| @@ -827,6 +816,7 @@ subroutine lsm_noah_run & ! end subroutine sfc_drv end subroutine lsm_noah_run !----------------------------------- +!! @} !! @} end module lsm_noah diff --git a/physics/sflx.f b/physics/sflx.f index e1b52a273..113b9b91f 100644 --- a/physics/sflx.f +++ b/physics/sflx.f @@ -9,8 +9,8 @@ !! and all terms of the surface energy balance and surface water balance !! (excluding input atmospheric forcings of downward radiation and precip). !! -!!\section general_sflx General Algorithm -!!\section detailed_sflx Detailed Algorithm +!\section general_sflx General Algorithm +!\section detailed_sflx Detailed Algorithm !----------------------------------- subroutine sflx & !................................... diff --git a/physics/tridi.f b/physics/tridi.f index dbf03e62b..38a408e7a 100644 --- a/physics/tridi.f +++ b/physics/tridi.f @@ -1,3 +1,10 @@ +!>\file tridi.f +!! These subroutines are originally internal subroutines in moninedmf.f + +!>\ingroup GFS_edmf_main +!!\brief Routine to solve the tridiagonal system to calculate +!!temperature and moisture at \f$ t + \Delta t \f$; part of two-part +!!process to calculate time tendencies due to vertical diffusion. subroutine tridi2(l,n,cl,cm,cu,r1,r2,au,a1,a2) cc use machine , only : kind_phys @@ -38,7 +45,10 @@ subroutine tridi2(l,n,cl,cm,cu,r1,r2,au,a1,a2) end c----------------------------------------------------------------------- - +!>\ingroup GFS_edmf_main +!! \brief Routine to solve the tridiagonal system to calculate u- and +!! v-momentum at \f$ t + \Delta t \f$; part of two-part process to +!! calculate time tendencies due to vertical diffusion. subroutine tridin(l,n,nt,cl,cm,cu,r1,r2,au,a1,a2) cc use machine , only : kind_phys From e8d25577148724c7319bbf565433c7a3ce3a5cbf Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Mon, 5 Feb 2018 14:56:55 -0700 Subject: [PATCH 10/22] format fixes --- physics/gwdc.f | 12 ++++++------ physics/gwdps.f | 4 ++-- physics/mfdeepcnv.f | 6 ------ physics/mfshalcnv.f | 21 +++++++++++---------- physics/moninedmf.f | 19 ++++++++++--------- physics/sfc_drv.f | 25 +++++++++++++------------ physics/sfc_sice.f | 12 ++++++------ 7 files changed, 48 insertions(+), 51 deletions(-) diff --git a/physics/gwdc.f b/physics/gwdc.f index 4d0328368..c9f879413 100644 --- a/physics/gwdc.f +++ b/physics/gwdc.f @@ -69,13 +69,13 @@ module gwdc_pre ! \brief Brief description of the subroutine ! ! \section arg_table_gwdc_pre_init Argument Table -!! +! subroutine gwdc_pre_init () end subroutine gwdc_pre_init ! \brief Brief description of the subroutine ! -! \section arg_table_gwdc_pre_run Argument Table +!> \section arg_table_gwdc_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|--------------------------------------------------------------------------|---------------------------------------------------------------|-------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -146,7 +146,7 @@ end subroutine gwdc_pre_run ! \brief Brief description of the subroutine ! ! \section arg_table_gwdc_pre_finalize Argument Table -!! +! subroutine gwdc_pre_finalize () end subroutine gwdc_pre_finalize @@ -1530,13 +1530,13 @@ module gwdc_post ! \brief Brief description of the subroutine ! ! \section arg_table_gwdc_post_init Argument Table -!! +! subroutine gwdc_post_init() end subroutine gwdc_post_init ! \brief Brief description of the subroutine ! -! \section arg_table_gwdc_post_run Argument Table +!> \section arg_table_gwdc_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------------|--------------------------------------------------------------------------|------------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | default | in | F | @@ -1611,7 +1611,7 @@ end subroutine gwdc_post_run ! \brief Brief description of the subroutine ! ! \section arg_table_gwdc_post_finalize Argument Table -!! +! subroutine gwdc_post_finalize() end subroutine gwdc_post_finalize diff --git a/physics/gwdps.f b/physics/gwdps.f index 69f146b63..232962539 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -112,7 +112,7 @@ end subroutine gwdps_pre_init ! \ingroup GFS_ogwd ! \brief Brief description of the subroutine ! -! \section arg_table_gwdps_pre_run Argument Table +!> \section arg_table_gwdps_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-------------------------------------------------------------------------|------------------------------------------------------------------------------------------|---------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal dimension | count | 0 | integer | default | in | F | @@ -1366,7 +1366,7 @@ end subroutine gwdps_post_init ! \ingroup GFS_ogwd ! \brief Brief description of the subroutine -! \section arg_table_gwdps_post_run Argument Table +!> \section arg_table_gwdps_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------|------------------------------------------------------------------|-------|------|---------|-----------|--------|----------| !! | lssav | flag_diagnostics | flag for calculating diagnostic fields | flag | 0 | logical | default | in | F | diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 5f83a29e7..4bff8ee8a 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -89,9 +89,6 @@ module sasas_deep ! \brief Brief description of the subroutine ! ! \section arg_table_sasasdeep_init Argument Table -! | local var name | longname | description | units | rank | type | kind | intent | optional | -! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| -! subroutine sasasdeep_init end subroutine sasasdeep_init @@ -99,9 +96,6 @@ end subroutine sasasdeep_init ! \brief Brief description of the subroutine ! ! \section arg_table_sasasdeep_finalize Argument Table -! | local var name | longname | description | units | rank | type | kind | intent | optional | -! |----------------|-----------------------------------------------------------|------------------------------------|---------|------|---------|-----------|--------|----------| -! subroutine sasasdeep_finalize end subroutine sasasdeep_finalize diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 308602a0a..c40f93fcf 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -28,6 +28,7 @@ module sasas_shal !! !! \section intraphysics_deep Intraphysics Communication !! + ! \brief Brief description of the subroutine ! ! \section arg_table_sasasshal_init Argument Table @@ -1706,8 +1707,8 @@ end subroutine sasasshal_run ! \brief Brief description of the subroutine ! -! \section arg_table_sasasshal_init Argument Table -! +!> \section arg_table_sasasshal_init Argument Table +!! subroutine sasasshal_finalize end subroutine sasasshal_finalize @@ -1770,17 +1771,17 @@ subroutine sasasshal_post_run (frain, rain1, cnvc, cnvw, Model, & end subroutine sasasshal_post_run -!! \brief Brief description of the subroutine -!! -!! \section arg_table_sasasshal_post_init Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_post_init Argument Table +! subroutine sasasshal_post_init () end subroutine sasasshal_post_init -!! \brief Brief description of the subroutine -!! -!! \section arg_table_sasasshal_post_finalize Argument Table -!! +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_post_finalize Argument Table +! subroutine sasasshal_post_finalize () end subroutine sasasshal_post_finalize diff --git a/physics/moninedmf.f b/physics/moninedmf.f index ca19993ed..56a66d8aa 100644 --- a/physics/moninedmf.f +++ b/physics/moninedmf.f @@ -6,13 +6,6 @@ module edmf contains -!> \defgroup HEDMF GFS Hybrid Eddy-diffusivity Mass-flux PBL and Free Atmospheric Turbulence -!! @{ -!! \brief The Hybrid EDMF scheme is a first-order turbulent transport scheme used for subgrid-scale vertical turbulent mixing in the PBL and above. It blends the traditional first-order approach that has been used and improved over the last several years with a more recent scheme that uses a mass-flux approach to calculate the countergradient diffusion terms. -!! -!! The PBL scheme's main task is to calculate tendencies of temperature, moisture, and momentum due to vertical diffusion throughout the column (not just the PBL). The scheme is an amalgamation of decades of work, starting from the initial first-order PBL scheme of Troen and Mahrt (1986) \cite troen_and_mahrt_1986, implemented according to Hong and Pan (1996) \cite hong_and_pan_1996 and modified by Han and Pan (2011) \cite han_and_pan_2011 and Han et al. (2015) \cite han_et_al_2015 to include top-down mixing due to stratocumulus layers from Lock et al. (2000) \cite lock_et_al_2000 and replacement of counter-gradient terms with a mass flux scheme according to Siebesma et al. (2007) \cite siebesma_et_al_2007 and Soares et al. (2004) \cite soares_et_al_2004. Recently, heating due to TKE dissipation was also added according to Han et al. (2015) \cite han_et_al_2015. -!! -!! \section intraphysics Intraphysics Communication subroutine edmf_init () end subroutine edmf_init @@ -20,6 +13,14 @@ end subroutine edmf_init subroutine edmf_finalize () end subroutine edmf_finalize +!> \defgroup HEDMF GFS Hybrid Eddy-diffusivity Mass-flux PBL and Free Atmospheric Turbulence +!> @{ +!! \brief The Hybrid EDMF scheme is a first-order turbulent transport scheme used for subgrid-scale vertical turbulent mixing in the PBL and above. It blends the traditional first-order approach that has been used and improved over the last several years with a more recent scheme that uses a mass-flux approach to calculate the countergradient diffusion terms. +!! +!! The PBL scheme's main task is to calculate tendencies of temperature, moisture, and momentum due to vertical diffusion throughout the column (not just the PBL). The scheme is an amalgamation of decades of work, starting from the initial first-order PBL scheme of Troen and Mahrt (1986) \cite troen_and_mahrt_1986, implemented according to Hong and Pan (1996) \cite hong_and_pan_1996 and modified by Han and Pan (2011) \cite han_and_pan_2011 and Han et al. (2015) \cite han_et_al_2015 to include top-down mixing due to stratocumulus layers from Lock et al. (2000) \cite lock_et_al_2000 and replacement of counter-gradient terms with a mass flux scheme according to Siebesma et al. (2007) \cite siebesma_et_al_2007 and Soares et al. (2004) \cite soares_et_al_2004. Recently, heating due to TKE dissipation was also added according to Han et al. (2015) \cite han_et_al_2015. +!! +!! \section intraphysics Intraphysics Communication +!! !>\defgroup GFS_edmf_main GFS moninedmf Main !> \brief This subroutine contains all of logic for the Hybrid EDMF PBL scheme except for the calculation of the updraft properties and mass flux. !! @@ -1195,7 +1196,8 @@ subroutine edmf_run (ix,im,km,ntrac,ntcw,dv,du,tau,rtg, & !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! return end subroutine edmf_run -!> @} +!! @} +!> @} c----------------------------------------------------------------------- ! \ingroup HEDMF @@ -1310,5 +1312,4 @@ end subroutine edmf_run C----------------------------------------------------------------------- C return C end -!> @} end module edmf diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index b178585e5..d0c40cdf2 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -59,10 +59,10 @@ !! !!\section Intraphysics Intraphysics Communication !! -!! \defgroup NOAH_pre NOAH Land Surface Pre -!! \ingroup NOAH -!! \brief Brief description of the parameterization -!! @{ +! \defgroup NOAH_pre NOAH Land Surface Pre +! \ingroup NOAH +! \brief Brief description of the parameterization +! @{ module lsm_noah_pre contains @@ -122,13 +122,13 @@ end subroutine lsm_noah_pre_run end module lsm_noah_pre -!! @} +! @} -!! \defgroup NOAH_post NOAH Land Surface post -!! \ingroup NOAH -!! @{ -!! \brief Brief description of the parameterization -!! \section intraphysics Intraphysics Communication +! \defgroup NOAH_post NOAH Land Surface post +! \ingroup NOAH +! @{ +! \brief Brief description of the parameterization +! \section intraphysics Intraphysics Communication module lsm_noah_post contains @@ -138,8 +138,8 @@ end subroutine lsm_noah_post_init subroutine lsm_noah_post_finalize end subroutine lsm_noah_post_finalize -!! \brief Brief description of the subroutine -!! +! \brief Brief description of the subroutine +! !! \section arg_table_lsm_noah_post_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|-------------------------------------------------------------|--------------------------------------------|------------|------|---------|-----------|--------|----------| @@ -300,6 +300,7 @@ end subroutine lsm_noah_finalize !----------------------------------- ! subroutine sfc_drv & + !> \defgroup NOAH_drv GFS sfc_drv Main !! \ingroup NOAH !! @{ diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index a0f13aa0a..7bfd3663e 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -776,19 +776,19 @@ module sfc_sice_pre !! ! \brief This subroutine is empty since there are no procedures needed ! \section arg_table_sfc_sice_pre_init Argument Table -!! +! subroutine sfc_sice_pre_init end subroutine sfc_sice_pre_init !! ! \brief This subroutine is empty since there are no procedures needed ! \section arg_table_sfc_sice_pre_finalize Argument Table -!! +! subroutine sfc_sice_pre_finalize end subroutine sfc_sice_pre_finalize -!! \section arg_table_sfc_sice_pre_run Argument Table +!> \section arg_table_sfc_sice_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------------|-------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -842,20 +842,20 @@ module sfc_sice_post !! ! \brief This subroutine is empty since there are no procedures needed ! \section arg_table_sfc_sice_post_init Argument Table -!! +! subroutine sfc_sice_post_init end subroutine sfc_sice_post_init !! ! \brief This subroutine is empty since there are no procedures needed ! \section arg_table_sfc_sice_post_finalize Argument Table -!! +! subroutine sfc_sice_post_finalize end subroutine sfc_sice_post_finalize !! -!! \section arg_table_sfc_sice_post_run Argument Table +!> \section arg_table_sfc_sice_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-------------------------------------------------------|---------------------------------------------|---------------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | From dc0cd17d939599226acbd4a6d665191e6aff30b0 Mon Sep 17 00:00:00 2001 From: "Man.Zhang" Date: Tue, 6 Feb 2018 11:19:17 -0700 Subject: [PATCH 11/22] doxy fix --- physics/mfdeepcnv.f | 1 - physics/mfshalcnv.f | 1 - physics/sfc_sice.f | 2 +- 3 files changed, 1 insertion(+), 3 deletions(-) diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 4bff8ee8a..3341ef076 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -1233,7 +1233,6 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & !! function, \f$z_0\f$ and \f$z_t\f$ are cloud base and cloud top, !! respectively, \f$\gamma = \frac{L}{c_p}\left(\frac{\partial \overline{q_s}}{\partial T}\right)_p\f$ !! and other quantities are previously defined. - do i = 1, im do i = 1, im if (cnvflg(i)) then aa1(i) = 0. diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index c40f93fcf..32b874cc2 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -997,7 +997,6 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & !! \f$z_0\f$ and \f$z_t\f$ are cloud base and cloud top, respectively, !! \f$\gamma = \frac{L}{c_p}\left(\frac{\partial \overline{q_s}}{\partial T}\right)_p\f$ !! and other quantities are previously defined. - do i = 1, im do i = 1, im if (cnvflg(i)) then aa1(i) = 0. diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 7bfd3663e..c57fb7298 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -143,7 +143,7 @@ subroutine sfc_sice_run & ! ! ! subprogram called: ice3lay. ! ! ! -u program history log: ! +! program history log: ! ! 2005 -- xingren wu created from original progtm and added ! ! two-layer ice model ! ! 200x -- sarah lu added flag_iter ! From 717c6f89ef7f9c23c3d16af70382700cbee120c6 Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Tue, 6 Feb 2018 11:40:49 -0700 Subject: [PATCH 12/22] fix SAMF doxygen --- physics/mfdeepcnv.f | 39 +++++++++++++++++++-------------------- physics/mfshalcnv.f | 3 ++- 2 files changed, 21 insertions(+), 21 deletions(-) diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 3341ef076..4ec32240c 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -52,21 +52,33 @@ !! to more strongly suppress convection in a drier environment. !! !! \section intraphysics Intraphysics Communication -!! This space is reserved for a description of how this scheme uses information -!! from other scheme types and/or how information calculated in this scheme -!! is used in other scheme types. +!! module sasas_deep contains + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasdeep_init Argument Table + subroutine sasasdeep_init + end subroutine sasasdeep_init + + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasdeep_finalize Argument Table + subroutine sasasdeep_finalize + end subroutine sasasdeep_finalize + !>\defgroup GFS_mfdeep GFS mfdeepcnv Main !!\ingroup SAMF !> @{ !>\brief This subroutine contains the entirety of the SAMF deep convection scheme. -!! -!! For grid sizes larger than threshold value, as in Grell (1993) -!! \cite grell_1993 , the SAMF deep convection scheme can be described -!! in terms of three types of "controls": static, dynamic, and feedback. +!! +!! For grid sizes larger than threshold value, as in Grell (1993) +!! \cite grell_1993 , the SAMF deep convection scheme can be described +!! in terms of three types of "controls": static, dynamic, and feedback. !! The static control component consists of the simple entraining/detraining !! updraft/downdraft cloud model and is used to determine the cloud !! properties, convective precipitation, as well as the convective cloud @@ -86,19 +98,6 @@ module sasas_deep !! in turn, determines changes of the large-scale environment due to the !! cumulus convection. !! -! \brief Brief description of the subroutine -! -! \section arg_table_sasasdeep_init Argument Table - subroutine sasasdeep_init - end subroutine sasasdeep_init - - -! \brief Brief description of the subroutine -! -! \section arg_table_sasasdeep_finalize Argument Table - subroutine sasasdeep_finalize - end subroutine sasasdeep_finalize - !! \section arg_table_sasasdeep_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------|-----------------------------------------------------|---------|------|---------|-----------|--------|----------| diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 32b874cc2..61e6db260 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -39,6 +39,7 @@ end subroutine sasasshal_init !>\defgroup SAMF_shal_main GFS mfshalcnv Main !!\ingroup SAMF_shal !> \brief The subroutine contains the entirety of the SAMF shallow convection scheme. +!! !! This routine follows the \ref SAMF deep scheme quite closely, although !! it can be interpreted as only having the "static" and "feedback" control !! portions, since the "dynamic" control is not necessary to find the @@ -1717,7 +1718,7 @@ end module sasas_shal module sasas_shal_post contains -!! \brief Brief description of the subroutine +!> \brief Brief description of the subroutine !! !! \section arg_table_sasasshal_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | From 11b71a90bd14d644f4a8497fe964c8d99715ae7b Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Fri, 9 Feb 2018 11:56:50 -0700 Subject: [PATCH 13/22] a new doc with bootstrapped stylesheet --- physics/docs/bootstrapped/customdoxygen.css | 370 ++++++++++++++++++++ physics/docs/bootstrapped/doxy-boot.js | 271 ++++++++++++++ physics/docs/bootstrapped/footer.html | 26 ++ physics/docs/bootstrapped/header.html | 42 +++ physics/docs/ccpp_dox | 37 +- physics/docs/ccpp_dox_Feb08 | 339 ++++++++++++++++++ physics/docs/txt/GFS_CALPRECIPTYPE.txt | 14 + physics/docs/txt/GFS_GWDC.txt | 68 ++++ physics/docs/txt/GFS_GWDPS.txt | 101 ++++++ physics/docs/txt/GFS_HEDMF.txt | 28 ++ physics/docs/txt/GFS_NOAH.txt | 62 ++++ physics/docs/txt/GFS_NSST.txt | 32 ++ physics/docs/txt/GFS_OZPHYS.txt | 21 ++ physics/docs/txt/GFS_RRTMG.txt | 112 ++++++ physics/docs/txt/GFS_SAMFdeep.txt | 66 ++++ physics/docs/txt/GFS_SAMFshal.txt | 36 ++ physics/docs/txt/GFS_SFCLYR.txt | 87 +++++ physics/docs/txt/GFS_SFCSICE.txt | 58 +++ physics/docs/txt/GFS_ZHAOC.txt | 70 ++++ physics/docs/txt/mainpage.txt | 79 ++--- physics/docs/txt/mainpage.txt.ORIG | 48 +++ physics/docs/txt/mainpage_bootstrapped.txt | 33 ++ physics/gwdps.f | 1 + physics/mfdeepcnv.f | 2 +- physics/radsw_main.f | 2 +- physics/sfc_nst.f | 1 - physics/sfc_sice.f | 2 +- 27 files changed, 1947 insertions(+), 61 deletions(-) create mode 100755 physics/docs/bootstrapped/customdoxygen.css create mode 100755 physics/docs/bootstrapped/doxy-boot.js create mode 100755 physics/docs/bootstrapped/footer.html create mode 100755 physics/docs/bootstrapped/header.html create mode 100644 physics/docs/ccpp_dox_Feb08 create mode 100644 physics/docs/txt/GFS_CALPRECIPTYPE.txt create mode 100644 physics/docs/txt/GFS_GWDC.txt create mode 100644 physics/docs/txt/GFS_GWDPS.txt create mode 100644 physics/docs/txt/GFS_HEDMF.txt create mode 100644 physics/docs/txt/GFS_NOAH.txt create mode 100644 physics/docs/txt/GFS_NSST.txt create mode 100644 physics/docs/txt/GFS_OZPHYS.txt create mode 100644 physics/docs/txt/GFS_RRTMG.txt create mode 100644 physics/docs/txt/GFS_SAMFdeep.txt create mode 100644 physics/docs/txt/GFS_SAMFshal.txt create mode 100644 physics/docs/txt/GFS_SFCLYR.txt create mode 100644 physics/docs/txt/GFS_SFCSICE.txt create mode 100644 physics/docs/txt/GFS_ZHAOC.txt create mode 100644 physics/docs/txt/mainpage.txt.ORIG create mode 100644 physics/docs/txt/mainpage_bootstrapped.txt diff --git a/physics/docs/bootstrapped/customdoxygen.css b/physics/docs/bootstrapped/customdoxygen.css new file mode 100755 index 000000000..c20bd11ba --- /dev/null +++ b/physics/docs/bootstrapped/customdoxygen.css @@ -0,0 +1,370 @@ +h1, .h1, h2, .h2, h3, .h3{ + font-weight: 200 !important; 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txt/GFS_SAMFdeep.txt \ + txt/GFS_SAMFshal.txt \ + txt/GFS_HEDMF.txt \ + txt/GFS_ZHAOC.txt \ + txt/GFS_SFCLYR.txt \ + txt/GFS_SFCSICE.txt \ + txt/GFS_NOAH.txt \ + txt/GFS_NSST.txt \ + txt/GFS_GWDPS.txt \ + txt/GFS_GWDC.txt \ + txt/GFS_OZPHYS.txt \ + txt/GFS_CALPRECIPTYPE.txt \ ### Radiation ../radiation_aerosols.f \ ../radiation_astronomy.f \ @@ -177,11 +190,11 @@ IGNORE_PREFIX = GENERATE_HTML = YES HTML_OUTPUT = html HTML_FILE_EXTENSION = .html -HTML_HEADER = -HTML_FOOTER = +HTML_HEADER = ./bootstrapped/header.html +HTML_FOOTER = ./bootstrapped/footer.html HTML_STYLESHEET = -HTML_EXTRA_STYLESHEET = ccpp_dox_extra_style.css -HTML_EXTRA_FILES = +HTML_EXTRA_STYLESHEET = ./bootstrapped/customdoxygen.css +HTML_EXTRA_FILES = ./bootstrapped/doxy-boot.js HTML_COLORSTYLE_HUE = 220 HTML_COLORSTYLE_SAT = 100 HTML_COLORSTYLE_GAMMA = 80 @@ -211,7 +224,7 @@ QHG_LOCATION = GENERATE_ECLIPSEHELP = NO ECLIPSE_DOC_ID = org.doxygen.Project DISABLE_INDEX = YES -GENERATE_TREEVIEW = YES +GENERATE_TREEVIEW = 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txt/GFS_CALPRECIPTYPE.txt \ +### Radiation + ../radiation_aerosols.f \ + ../radiation_astronomy.f \ + ../radiation_clouds.f \ + ../radiation_gases.f \ + ../radiation_surface.f \ + ../radlw_datatb.f \ + ../radlw_main.f \ + ../radlw_param.f \ + ../radsw_datatb.f \ + ../radsw_main.f \ + ../radsw_param.f \ + ../GFS_radupdate.f90 \ +### Deep Convection + ../mfdeepcnv.f \ +### Shallow Convection + ../mfshalcnv.f \ +### PBL + ../moninedmf.f \ + ../mfpbl.f \ + ../tridi.f \ +### Microphysics + ../precpd.f \ + ../gscond.f \ +### Land Surface + ../sfc_drv.f \ + ../sflx.f \ + ../sfcsub.f \ + ../sfc_diff.f \ + ../set_soilveg.f \ + ../GFS_calpreciptype.f90 \ +### Sea Ice Surface + ../sfc_sice.f \ +### Ocean Surface + ../sfc_nst.f \ +### Orographic Gravity Wave + ../gwdps.f \ +### Convective Gravity Wave + ../gwdc.f \ +### Rayleigh damp + ../rayleigh_damp.f \ +### Prognostic Ozone + ../ozphys.f +INPUT_ENCODING = UTF-8 +FILE_PATTERNS = *.f \ + *.txt +RECURSIVE = YES +EXCLUDE = +EXCLUDE_SYMLINKS = NO 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b/physics/docs/txt/GFS_CALPRECIPTYPE.txt new file mode 100644 index 000000000..7cef46794 --- /dev/null +++ b/physics/docs/txt/GFS_CALPRECIPTYPE.txt @@ -0,0 +1,14 @@ +/** +\page GFS_CALPRECIPTYPE GFS Dominant Precipitation Scheme +\section des_calprecip 1. Description +This scheme calculates dominant precipitation type (calpreciptype), +which provides precipitation forcing for LSM. + +\section intra_calprecip 2. Intraphysics Communication +\ref arg_table_GFS_calpreciptype_run + +\section gen_calprecip 3. General Algorithm + + + +*/ diff --git a/physics/docs/txt/GFS_GWDC.txt b/physics/docs/txt/GFS_GWDC.txt new file mode 100644 index 000000000..08926e5cb --- /dev/null +++ b/physics/docs/txt/GFS_GWDC.txt @@ -0,0 +1,68 @@ +/** +\page GFS_GWDC GFS Convective Gravity Wave Drag Scheme +\section des_gwdc 1. Description + The GFS orographic gravity wave drag parameterization calculates the + effect of gravity waves produced by uneven distribution of diabatic + heat sources asscociated with convective systems on the + horizontal wind. + + At present, global models must be run with horizontal resolutions + that cannot typically resolve atmospheric phenomena shorter than + ~10-100 km or greater for weather prediction and ~100-1000 km or + greater for climate predicition. Many atmospheric processes have + shorter horizontal scales than these "subgrid-scale" processes + interact with and affect the larger-scale atmosphere in important + ways. + + Atmospheric gravity waves are one such unresolved processes. These + waves are generated by lower atmospheric sources. e.g., flow over + irregularities at the Earth's surface such as mountains and valleys, + uneven distribution of diabatic heat sources asscociated with + convective systems, and highly dynamic atmospheric processes such + as jet streams and fronts. The dissipation of these waves produces + synoptic-scale body forces on the atmospheric flow, known as + "gravity wave drag"(GWD), which affects both short-term evolution + of weather systems and long-term climate. However, the spatial + scales of these waves (in the range of ~5-500 km horizontally) are + too short to be fully captured in models, and so GWD must be + parameterized. In addition, the role of GWD in driving the global + middle atmosphere circulation and thus global mean wind/temperature + structures is well established. Thus, GWD parametrizations are now + critical components of virtually all large-scale atmospheric models. + GFS physics includes parameterizations of gravity waves from two + important sources: mountains and convection. This parameterization + addresses the latter. + + In a review paper on gravity waves in the middle atmosphere, Fritts + (1984) \cite fritts_1984 showed that a large portion of observed + gravity wave momentum flux has higher frequencies than those of + stationary mountain waves. This phenomenon was explained by cumulus + convection, which is an additional source of tropospheric gravity + waves, and is particularly important in summertime. When the surface + wind and stability are weak, the magnitude of the surface drag and + the resultant influence of orographically-induced gravity wave drag + on the large-scale flow are relatively small compared with those in + wintertime (Palmer et al. 1986 \cite palmer_et_al_1986). In this + situation, the relative importance of cumulus convection as a source + of gravity waves is larger. In addition, in the tropical regions + where persistent convection exists, deep cumulus clouds impinging on + the stable stratosphere can generate gravity waves that influence + the large-scale flow. + +\subsection provenance_gwdc Provenance + The parameterization of stationary convectively-forced GWD follows + the development of Chun and Baik (1998) \cite chun_and_baik_1998 , + which was tested in GCMs by Chun et al. (2001,2004) + \cite chun_et_al_2001 \cite chun_et_al_2004 was implemented in GFS + by Ake Johansson (2008) and the work of the GCWMB staff. Modest + positive effects from using the parameterization are seen in the + tropical upper troposphere and lower stratosphere. + +\section intra_gwdc 2. Intraphysics Communication +\ref arg_table_gwdc_run + +\section gen_gwdc 3. General Algorithm + + + +*/ diff --git a/physics/docs/txt/GFS_GWDPS.txt b/physics/docs/txt/GFS_GWDPS.txt new file mode 100644 index 000000000..29f78a708 --- /dev/null +++ b/physics/docs/txt/GFS_GWDPS.txt @@ -0,0 +1,101 @@ +/** +\page GFS_GWDPS GFS Orographic Gravity Wave Drag Scheme +\section des_gwdps 1. Description + The GFS orographic gravity wave drag parameterization calculates the + effect of gravity waves produced by flow over irregularities at the + Earth's surface such as mountains and valleys and highly dynamic + atmospheric processes such as jet streams and fronts on the + horizontal wind. At present, global models must be run with horizontal resolutions + that cannot typically resolve atmospheric phenomena shorter than + ~10-100 km or greater for weather prediction and ~100-1000 km or + greater for climate predicition. Many atmospheric processes have + shorter horizontal scales than these "subgrid-scale" processes + interact with and affect the larger-scale atmosphere in important + ways. + + Atmospheric gravity waves are one such unresolved processes. These + waves are generated by lower atmospheric sources. e.g., flow over + irregularities at the Earth's surface such as mountains and valleys, + uneven distribution of diabatic heat sources asscociated with + convective systems, and highly dynamic atmospheric processes such + as jet streams and fronts. The dissipation of these waves produces + synoptic-scale body forces on the atmospheric flow, known as + "gravity wave drag"(GWD), which affects both short-term evolution + of weather systems and long-term climate. However, the spatial + scales of these waves (in the range of ~5-500 km horizontally) are + too short to be fully captured in models, and so GWD must be + parameterized. In addition, the role of GWD in driving the global + middle atmosphere circulation and thus global mean wind/temperature + structures is well established. Thus, GWD parametrizations are now + critical components of virtually all large-scale atmospheric models. + GFS physics includes parameterizations of gravity waves from two + important sources: mountains and convection. This parameterization + address the former. + + Atmospheric flow is significantly influenced by orography creating + lift and frictional forces. The representation of orography and its + influence in numerical weather prediction models are necessarily + divided into the resolvable scales of motion and treated by + primitive equations, the remaining sub-grid scales to be treated by + parameterization. In terms of large scale NWP models, mountain + blocking of wind flow around sub-grid scale orograph is a process + that retards motion at various model vertical levels near or in the + boundary layer. Flow around the mountain encounters larger + frictional forces by being in contact with the mountain surfaces + for longer time as well as the interaction of the atmospheric + environment with vortex shedding which occurs in numerous + observations. Lott and Miller (1997) \cite lott_and_miller_1997, + incorporated the dividing streamline and mountain blocking in + conjunction with sub-grid scale vertically propagating gravity wave + parameterization in the context of NWP. The dividing streamline is + seen as a source of gravity waves to the atmosphere above and + nonlinear subgrid low-level mountain drag effect below. + + \subsection provenance_gwdps Provenance + - Gravity-wave drag is simulated as described by Alpert et al. + (1988) \cite alpert_et_al_1988. The parameterization includes + determination of the momentum flux due to gravity waves at the + surface, as well as upper levels. The surface stress is a nonlinear + function of the surface wind speed and the local Froude number, + following Pierrehumbert (1987) \cite pierrehumbert_1987. Vertical + variations in the momentum flux occur when the local Richardson + number is less than 0.25 (the stress vanishes), or when wave + breaking occurs (local Froude number becomes critical); in the + latter case, the momentum flux is reduced according to the + Lindzen(1981) \cite lindzen_1981 wave saturation hypothesis. + Modifications are made to avoid instability when the critical layer + is near the surface, since the time scale for gravity-wave drag is + shorter than the model time step. + + - The treatment of the GWD in the lower troposphere is enhanced + according to Kim and Arakawa (1995) \cite kim_and_arakawa_1995 . + Orographic Std Dev (HPRIME), Convexity(OC), Asymmetry (OA4) and Lx + (CLX4) are input topographic statistics needed (see Appendix in Kim + and Arakawa (1995) \cite kim_and_arakawa_1995) . + + - Mountain blocking influences are incorporated following the Lott + and Miller (1997) \cite lott_and_miller_1997 parameterization with + minor changes, including their dividing streamline concept. The + model subgrid scale orography is represented by four parameters, + after Baines and Palmer (1990) \cite baines_and_palmer_1990, the + standard deviation (HPRIME), the anisotropy (GAMMA), the slope + (SIGMA) and the geographical orientation of the orography (THETA). + These are calculated off-line as a function of model resolution in + the fortran code ml01rg2.f, with script mlb2.sh (see Appendix: + Specification of subgrid-scale orography in Lott and Miller (1997) + \cite lott_and_miller_1997). + + - The orographic GWD parameterizations automatically scales + with model resolution. For example, the T574L64 version of GFS uses + four times stronger mountain blocking and one half the strength of + gravity wave drag than the T383L64 version. + + +\section intra_gwdps 2. Intraphysics Communication +\ref arg_table_gwdps_run + +\section gen_al_gwdps 3. General Algorithm + + + +*/ diff --git a/physics/docs/txt/GFS_HEDMF.txt b/physics/docs/txt/GFS_HEDMF.txt new file mode 100644 index 000000000..b0e03ea95 --- /dev/null +++ b/physics/docs/txt/GFS_HEDMF.txt @@ -0,0 +1,28 @@ +/** +\page GFS_HEDMF GFS Hybrid Eddy-Diffusivity Mass-Flux PBL and Free Atmospheric Turbulence Scheme +\section des_pbl 1. Description +The Hybrid EDMF scheme is a first-order turbulent transport scheme used for subgrid-scale vertical turbulent mixing in the PBL and above. It blends the traditional first-order approach that has been used and improved over the last several years with a more recent scheme that uses a mass-flux approach to calculate the countergradient diffusion terms. + +The PBL scheme's main task is to calculate tendencies of temperature, moisture, and momentum due to vertical diffusion throughout the column (not just the PBL). The scheme is an amalgamation of decades of work, starting from the initial first-order PBL scheme of Troen and Mahrt (1986) \cite troen_and_mahrt_1986, implemented according to Hong and Pan (1996) \cite hong_and_pan_1996 and modified by Han and Pan (2011) \cite han_and_pan_2011 and Han et al. (2015) \cite han_et_al_2015 to include top-down mixing due to stratocumulus layers from Lock et al. (2000) \cite lock_et_al_2000 and replacement of counter-gradient terms with a mass flux scheme according to Siebesma et al. (2007) \cite siebesma_et_al_2007 and Soares et al. (2004) \cite soares_et_al_2004. Recently, heating due to TKE dissipation was also added according to Han et al. (2015) \cite han_et_al_2015. + +The scheme works on a basic level by calculating background diffusion coefficients and updating them according to which processes are occurring in the column. The most important difference in diffusion coefficients occurs between those levels in the PBL and those above the PBL, so the PBL height calculation is of utmost importance. An initial estimate is calculated in a "predictor" step in order to calculate Monin-Obukhov similarity values and a corrector step recalculates the PBL height based on updated surface thermal characteristics. Using the PBL height and the similarity parameters, the diffusion coefficients are updated below the PBL top based on Hong and Pan (1996) \cite hong_and_pan_1996 (including counter-gradient terms). Diffusion coefficients in the free troposphere (above the PBL top) are calculated according to Louis (1979) \cite louis_1979 with updated Richardson number-dependent functions. If it is diagnosed that PBL top-down mixing is occurring according to Lock et al. (2000) \cite lock_et_al_2000 , then then diffusion coefficients are updated accordingly. Finally, for convective boundary layers (defined as when the Obukhov length exceeds a threshold), the counter-gradient terms are replaced using the mass flux scheme of Siebesma et al. (2007) \cite siebesma_et_al_2007 . In order to return time tendencies, a fully implicit solution is found using tridiagonal matrices, and time tendencies are "backed out." Before returning, the time tendency of temperature is updated to reflect heating due to TKE dissipation following Han et al. (2015) \cite han_et_al_2015 . + +This scheme includes the following subroutines: ++ edmf::edmf_run() ++ tridi2() ++ tridin() ++ mfpbl() + +\section intra_pbl 2. Intraphysics Communication +\sa \ref arg_table_edmf_run + +\section gen_pbl 3. General Algorithm +\sa \ref general_edmf + +\section det_pbl 4. Detailed Algorithm +\sa \ref detailed_edmf + + + + +*/ diff --git a/physics/docs/txt/GFS_NOAH.txt b/physics/docs/txt/GFS_NOAH.txt new file mode 100644 index 000000000..547898075 --- /dev/null +++ b/physics/docs/txt/GFS_NOAH.txt @@ -0,0 +1,62 @@ +/** +\page GFS_NOAH GFS Noah Land Surface Scheme +\section des_noah 1. Description + Land-atmosphere interactions are a main driver of Earth's surface + water and energy budgets. The importance of the land surface is + rather intuitive, and has been demonstrated not only in terms of + predictability on daily to seasonal timescale (Betts et al. 2017 + \cite betts_et_al_2017), but also in terms + of influencing extremes such as drought and heatwaves (PaiMazumder and + Done, 2016 \cite paimazumder_and_done_2016), PBL evolution and cloud + formation (Milovac et al. 2016 \cite milovac_et_al_2016) and afternoon + convection (Guillod et al. 2015 \cite guillod_et_al_2015), and + tropical cyclone re-intensification (Andersen and Shepherd, 2014 + \cite andersen_and_shepherd_2014). Other linkages, such as the role of soil + moisture (SM) or vegetation heterogeneity in mesoscale circulation + (Hsu et al. 2017 \cite hsu_et_al_2017) and planetary waves (Koster + et al. 2014 \cite koster_et_al_2014), and those driven by land use + and land cover change or management (Hirsch et al. 2015 + \cite hirsch_et_al_2015, Findell et al. 2017 + \cite findell_et_al_2017) are topics of active research. + + Figure 1 is a schematic of local land-atmosphere interactions in a + quiescent synoptic regime, including the soil moisture-precipitation + (SM-P) feedback pathways. Solid arrows indicate a positive feedback + pathway, and large dashed arrows represent a negative feedback, while + red indicates radiative, black indicates surface layer and PBL, and + brown indicates land surface processes. Thin red and grey dashed lines + with arrows also represent positive feedbacks. The single horizontal + gay-dotted line (no arrows) indicates the top of the PBL, and the seven + small vertical dashed lines (no arrows) represent precipitation + \image html Noah_LA_interaction.png "Figure 1: Local Land-atmosphere Interaction (courtesy of Micheal Ek, Ek and Mahrt (1994), Ek and Holtslag (2004))" width=10cm + The land-surface model component was substantially upgraded from the Oregon + State University (OSU) land surface model to EMC's new NOAH Land Surface Model + (NOAH LSM) during the major implementation in the NCEP Global Forecast System + (GFS) on May 31, 2005. Forecast System (GFS). The NOAH LSM embodies about 10 + years of upgrades (see Chen et al. 1996 + \cite chen_et_al_1996; Koren et al. 1999 \cite koren_et_al_1999; Ek et al. 2003 + \cite ek_et_al_2003) to its ancestor, the OSU LSM. The NOAH LSM upgrade includes: + - An increase from two (10, 190 cm thick) to four soil layers (10, 30, 60, 100 cm thick) + - Addition of frozen soil physics + - Add glacial ice treatment + - Two snowpack states (SWE, density) + - New formulations for infiltration and runoff account for sub-grid variability in precipitation and soil moisture + - Revised physics of the snowpack and its influence on surface heat fluxes and albedo + - Higher canopy resistance + - Spatially varying root depth + - Surface fluxes weighted by snow cover fraction + - Improved thermal conduction in soil/snow + - Improved seasonality of green vegetation cover. + - Improved evaporation treatment over bare soil and snowpack + + \image html land_dataset.png "Figure 2: Land Data Sets Used in NCEP Modeling Systems" width=10cm + + +\section intra_noah 2. Intraphysics Communication +\ref arg_table_lsm_noah_run + +\section gen_al_noah 3. General Algorithm + + + +*/ diff --git a/physics/docs/txt/GFS_NSST.txt b/physics/docs/txt/GFS_NSST.txt new file mode 100644 index 000000000..f8db1f130 --- /dev/null +++ b/physics/docs/txt/GFS_NSST.txt @@ -0,0 +1,32 @@ +/** +\page GFS_NSST GFS Near Sea Surface Temperature Scheme +\section des_nst 1. Description +Near Sea Surface Temperature (NSST) is a temperature profile just below the sea surface. The GFS NSST scheme is used to forecast the NSST for two main purposes: supply SSTs to the atmospheric model for the calculation of air-sea heat and moisture fluxes and providing a sub-layer temperature profile forecast for use as a first guess in the Gridpoint Statistical Interpolator (GSI) data assimilation code. + + The GFS NSST scheme was initially developed at NCEP by Xu Li in 2007, and subsequently received contributions by S. Moorthi, Y.-T. Hu and J. Derber, leading to operational implementation in the GFS in 2017 (Li 2015 \cite Li_2015, and Li and Derber 2009 \cite Li_Derber_2009). The GFS NSST scheme predicts the vertical profile of sea temperature between the surface and a reference level (zr), which is on the order of 5 m. Only two physical process are considered in this scheme: diurnal thermocline layer warming and thermal skin layer (also known as sub-layer) cooling. All other process that could influence NSST are ignored in this simple scheme. + +This profile is a composed by subdividing the near-surface layer in three parts + +T(z) = Tr + T’w (z) + T’c (z), + +where +Ts = T(z=0) is the SST +T’c (z) is the temperature profile in the skin layer (0 < z <= zc) +T’w (z) is the temperature profile in the warm layer (0 < z <= zr) +Tr is the reference temperature +zc is the depth of the skin layer + +Prediction for the skin layer is made using the Thermal Skin-layer Model (TSM), while prediction for the thermocline is based on the Diurnal Thermocline Model (DTM), both with an origin on Fairall et al. (1996) \cite Fairall_all_1996. Atmospheric inputs include short- and long-wave radiation, surface pressure, surface layer winds, temperature and specific humidity, and rainfall. + + \htmlonly + \endhtmlonly + @image html NSST.png "Figure 1: NSST profile." + +\section intra_nst 2. Intraphysics Communication +\ref arg_table_sfc_nst_run + +\section gen_nst 3. General Algorithm + + + +*/ diff --git a/physics/docs/txt/GFS_OZPHYS.txt b/physics/docs/txt/GFS_OZPHYS.txt new file mode 100644 index 000000000..e117e61ee --- /dev/null +++ b/physics/docs/txt/GFS_OZPHYS.txt @@ -0,0 +1,21 @@ +/** +\page GFS_OZPHYS GFS Ozone Sources and Sinks Scheme +\section des_ozone 1. Description + The operational GFS currently parameterizes ozone production and + destruction based on monthly mean coefficients provided by Naval + Research Laboratory through CHEM2D chemistry model + (McCormack et al. 2006 \cite mccormack_et_al_2006). + Monthly and zonal mean ozone production rate and ozone destruction + rate per unit ozone mixing ratio were provided by NRL based on + CHEM2D model. + Original version of these terms were provided by NASA/DAO based on + NASA 2D Chemistry model - GSM is capable of running both versions + +\section intra_ozone 2. Intraphysics Communication +\ref arg_table_ozphys_run + +\section gen_ozone 3. General Algorithm + + + +*/ diff --git a/physics/docs/txt/GFS_RRTMG.txt b/physics/docs/txt/GFS_RRTMG.txt new file mode 100644 index 000000000..7e3c3dca0 --- /dev/null +++ b/physics/docs/txt/GFS_RRTMG.txt @@ -0,0 +1,112 @@ +/** +\page GFS_RRTMG GFS RRTMG Shortwave/Longwave Radiation Scheme + +\section des_rrtmg 1. Description + Radiative processes are among the most complex and + computationally intensive parts of all model physics. As an + essential component of modeling the atmosphere, radiation directly + and indirectly connects all physics processes with model dynamics, + and it regulates the overall earth-atmosphere energy exchanges and + transformations. + + The schematic radiation module structure is shown in Table 1. + \image html schematic_Rad_mod.png "Table 1: Schematic Radiation Module Structure" width=10cm + + The links to each radiation module: + + @ref module_radlw_main + + @ref radlw_param + + @ref radlw_datatb + + @ref module_radsw_main + + @ref radsw_param + + @ref radsw_datatb + + @ref module_radiation_aerosols + + @ref module_radiation_astronomy + + @ref module_radiation_clouds + + @ref module_radiation_gases + + GFS radiation package is intended to provide a fast and accurate + method of determining the total radiative flux at any given + location. These calculations provide both the total radiative flux + at the ground surface, which is needed to establish the surface + energy budget, and the vertical radiative flux divergence, which is + used to calculate the radiative heating and cooling rates of a given + atmospheric layer. The magnitude of the terms in the surface energy + budget can set the stage for moist deep convection and are crucial + to the formation of low-level clouds. In addition, the vertical + radiative flux divergence can produce substantial cooling, + particularly at the tops of clouds, which can have strong dynamical + effects on cloud evolution. + + It uses a correlated-k distribution method and a transmittance lookup + table that is linearly scaled by optical depth to achieve high + accuracy and efficiency. The algorithm contains 140 unevenly + distributed quadrature points (reduced from the original set of 256) + to integrate the cumulative probability distribution functions of + absorption over 16 spectral bands. It employs the + Clough-Kneizys-Davies (CKD_2.4) continuum model (Clough et al. 1992 + \cite clough_et_al_1992) to compute absorption by water vapor at the + continuum band. Longwave cloud radiative properties external to the + RRTM depend on cloud liquid/ice water path and the effective radius + of ice particles and water droplets (Hu and Stamnes 1993 + \cite hu_and_stamnes_1993; Ebert and Curry 1992 \cite ebert_and_curry_1992). + + Changes to Radiation Parameterization since 2007: + \n The longwave (LW) and the shortwave (SW) radiation + parameterizations in NCEP's operational GFS are both modified and + optimized versions of the Rapid Radiative Transfer Model for GCMs + (RRTMG_LW v2.3 and RRTMG_SW v2.3, respectively) developed at AER + (Iacono et al. 2008 \cite iacono_et_al_2008,Mlawer et al. 1997 + \cite mlawer_et_al_1997, Iacono et al., 2000 \cite iacono_et_al_2000, + Clough et al., 2005 \cite clough_et_al_2005). The LW algorithm + contains 140 unevenly distributed g-points (quadrature points) in 16 + broad spectral bands, while the SW algorithm includes 112 g-points + in 14 bands. In addition to the major atmospheric absorbing gases of + ozone, water vapor, and carbon dioxide, the algorithm also includes + various minor absorbing species such as methane, nitrous oxide, + oxygen, and in the longwave up to four types of halocarbons (CFCs). + To represent statistically the unresolved subgrid cloud variability + when dealing multi layered clouds, a Monte-Carlo Independent Column + Approximation (McICA) method is used in the RRTMG radiative transfer. + A maximum-random cloud overlap method is used in both LW and SW + radiation calculations. Cloud condensate path and effective radius + for water and ice are used for the calculation of cloud-radiative + properties. Hu and Stamnes's method (1993) \cite hu_and_stamnes_1993 + is used to treat water clouds in both LW and SW parameterizations. + For ice clouds. Fu's parameterizations (1996,1998) \cite fu_1996 + \cite fu_et_al_1998 are used in the SW and LW, respectively. + + In the operational GFS, a climatological tropospheric aerosol with + a 5-degree horizontal resolution is used in both LW and SW + radiations. A generalized spectral mapping formulation was developed + to compute radiative properties of various aerosol components for + each of the radiation spectral bands. A separate stratospheric + volcanic aerosol parameterization was added that is capable of + handling volcanic events. In SW, a new table of incoming solar + constants is derived covering time period of 1850-2019 (Vandendool, + personal communivation). An eleven-year solar cycle approximation + will be used for time out of the window period in long term climate + simulations. The SW albedo parameterization uses surface vegetation + type based seasonal climatology similar to that described in the + NCEP OFFICE Note 441 (Hou et al. 2002 \cite hou_et_al_2002) but with + a modification in the treatment of solar zenith angle dependency over + snow-free land surface (Yang et al. 2008 \cite yang_et_al_2008). + Similarly, vegetation type based non-black-body surface emissivity + is used for the LW radiation. Concentrations of atmospheric + greenhouse gases are either obtained from global network + measurements, such as carbon dioxide (CO2), or taking the + climatological constants, the actual CO2 value for the forecast time + is an estimation based on the most recent five-year observations. In + the lower atmosphere (<3km) a monthly mean CO2 distribution in 15 + degree horizontal resolution is used, while a global mean monthly + value is used in the upper atmosphere. + +\section intraphysics_rrtmg 2. Intraphysics Communication + + For RRTMG-Longwave radiation parameterization: \sa \ref arg_table_lwrad_run + + For RRTMG-Shortwave radiation parameterization: \sa \ref arg_table_swrad_run + +\section gen_al_rrtmg 3. General Algorithm + + For RRTMG-Longwave radiation parameterization: \sa \ref gen_lwrad + + For RRTMG-Shortwave radiation parameterization: \sa \ref gen_swrad + + +*/ diff --git a/physics/docs/txt/GFS_SAMFdeep.txt b/physics/docs/txt/GFS_SAMFdeep.txt new file mode 100644 index 000000000..3180e8f3d --- /dev/null +++ b/physics/docs/txt/GFS_SAMFdeep.txt @@ -0,0 +1,66 @@ +/** +\page GFS_SAMFdeep GFS Scale-Aware Mass-Flux Deep Convection Scheme +\section des_deep 1. Description + The scale-aware mass-flux (SAMF) deep convection scheme is an + updated version of the previous Simplified Arakawa-Schubert (SAS) scheme + with scale and aerosol awareness and parameterizes the effect of deep + convection on the environment (represented by the model state variables) + in the following way. First, a simple cloud model is used to determine + the change in model state variables due to one entraining/detraining cloud + type, per unit cloud-base mass flux. Next, the total change in state variables + is retrieved by determining the actual cloud base mass flux using the + quasi-equilibrium assumption (for grid sizes larger than a threshold value + [currently set to 8 km]) or a mean updraft velocity (for grid sizes smaller + than the threshold value). With a scale-aware parameterization, the + cloud mass flux decreases with increasing grid resolution. A simple + aerosol-aware parameterization is employed, where rain conversion in + the convective updraft is modified by aerosol number concentration. + The name SAS is replaced with SAMF as for the smaller grid sizes, + the parameterization does not use Arakawa-Schubert's quasi-equilibrium + assumption any longer where the cloud work function (interpreted as + entrainment-moderated convective available potential energy [CAPE]) + by the large scale dynamics is in balance with the consumption of the + cloud work function by the convection. + + The SAS scheme uses the working concepts put forth in Arakawa and + Schubert (1974) \cite arakawa_and_schubert_1974 but includes modifications + and simplifications from Grell (1993) \cite grell_1993 such as saturated + downdrafts and only one cloud type (the deepest possible), rather than + a spectrum based on cloud top heights or assumed entrainment rates. + The scheme was implemented for the GFS in 1995 by Pan and Wu + \cite pan_and_wu_1995, with further modifications discussed in + Han and Pan (2011) \cite han_and_pan_2011 , including the calculation + of cloud top, a greater CFL-criterion-based maximum cloud base mass flux, + updated cloud model entrainment and detrainment, improved convective + transport of horizontal momentum, a more general triggering function, + and the inclusion of convective overshooting. + + The SAMF scheme updates the SAS scheme with scale- and aerosol-aware + parameterizations from Han et al. (2017) \cite han_et_al_2017 based on + the studies by Arakawa and Wu (2013) \cite arakawa_and_wu_2013 and + Grell and Freitas (2014) \cite grell_and_freitas_2014 for scale awareness + and by Lim (2011) \cite lim_2011 for aerosol awareness. The ratio of + advective time to convective turnover time is also taken into account + for the scale-aware parameterization. Along with the scale- and aerosol-aware + parameterizations, more changes are made to the SAMF scheme. The cloud + base mass-flux computation is modified to use convective turnover time + as the convective adjustment time scale. The rain conversion rate is + modified to decrease with decreasing air temperature above the freezing + level. Convective inhibition in the sub-cloud layer is used as an additional + trigger condition. Convective cloudiness is enhanced by considering suspended + cloud condensate in the updraft. The lateral entrainment is also enhanced + to more strongly suppress convection in a drier environment. + +\section intra_deep 2. Intraphysics Communication +\sa \ref arg_table_sasasdeep_run + +\section gen_al_deep 3. General Algorithm +\sa \ref general_mfdeep + +\section det_al_deep 4. Detailed Algorithm +\sa \ref detailed_deep + + + + +*/ diff --git a/physics/docs/txt/GFS_SAMFshal.txt b/physics/docs/txt/GFS_SAMFshal.txt new file mode 100644 index 000000000..e5337fe25 --- /dev/null +++ b/physics/docs/txt/GFS_SAMFshal.txt @@ -0,0 +1,36 @@ +/** +\page GFS_SAMFshal GFS Scale-Aware Mass-Flux Shallow Convection Scheme + +\section des_shal 1. Description + The scale-aware mass-flux shallow (SAMF_shal) convection + scheme is an updated version of the previous mass-flux shallow + convection scheme with scale and aerosol awareness and + parameterizes the effect of shallow convection on the environment. + The SAMF_shal scheme is similar to the SAMF deep convection scheme + but with a few key differences. First, no quasi-equilibrium assumption + is used for any grid size and the shallow cloud base mass flux is + parameterized using a mean updraft velocity. Further, there are no + convective downdrafts, the entrainment rate is greater than for deep + convection, and the shallow convection is limited to not extend over + the level where \f$p=0.7p_{sfc}\f$. The paramerization of scale and + aerosol awareness follows that of the SAMF deep convection scheme. + + The previous version of the shallow convection scheme (shalcnv.f) + is described in Han and Pan (2011) \cite han_and_pan_2011 and differences + between the shallow and deep convection schemes are presented in + Han and Pan (2011) \cite han_and_pan_2011 and Han et al. (2017) + \cite han_et_al_2017 . Details of scale- and aerosol-aware parameterizations + are described in Han et al. (2017) \cite han_et_al_2017 . + +\section intr_shal 2. Intraphysics Communication +\sa \ref arg_table_sasasshal_run + +\section gen_shal 3. General Algorithm +\sa \ref general_mfshal + +\section det_shal 4. Detailed Algorithm +\sa \ref detailed_mfshal + + + +*/ diff --git a/physics/docs/txt/GFS_SFCLYR.txt b/physics/docs/txt/GFS_SFCLYR.txt new file mode 100644 index 000000000..aa4002c0d --- /dev/null +++ b/physics/docs/txt/GFS_SFCLYR.txt @@ -0,0 +1,87 @@ +/** +\page GFS_SFCLYR GFS Surface Roughness Length Calculation +\section des_rough 1. Description + It is the surface roughness length formulation based on + the surface sublayer scheme from Zeng and Dickinson (1998) + \cite zeng_and_dickinson_1998. + + NOAH LSM are largely responsible for the quality + of model forecasts produced for near-surface weather parameters, such + as 2-meter air temperature (\a T2m) and surface skin temperature + (\a LST). LST is derived from the surface energy budget, and is + particularly important to remote sensing and data assimilation. How + precise these two parameters can be simulated by the model strongly + dependes on how accurate the surface heat fluxes are parameterized, + particularly the surface sensible heat flux (\a SH). The surface + thermal roughness length is a key parameter to determine \a SH. + Previous GFS version do not distinguish between the roughness length + for heat and momentum. The aerodynamic roughness \f$Z_{0m}\f$ is used + for wind, while the thermal roughness \f$Z_{0t}\f$ is used for heat and + water vapor. In general,\f$Z_{0m}\f$ is different from \f$Z_{0t}\f$, + because the transfer of momentum is affected by pressure fluctuations + in the turbulent waves behind the roughness elements, while for heat + and water vapor transfer no such dynamical mechanism exists. Zeng and + Dickinson (1998) \cite zeng_and_dickinson_1998 found that the surface + skin temperature can be at least 10 K higher when considering the surface + sublayer (or the variable ratio of the \f$Z_{0m}/Z_{0t}\f$ than without + in the desert summer afternoon. + + In May 2011, the new vegetation-dependent formulations of + momentum and thermal roughness formulation (Zheng et al. 2009 + \cite zheng_et_al_2009; Zheng et al. 2012 \cite zheng_et_al_2012 ) + was implemented to deal with the cold LST bias + over the arid western continental United States + (CONUS) during daytime. This LST bias contributes to large errors in + simulated satellite brightness temperatures over land by the Community + Radiative Transfer Model (CRTM) and hence the rejection of satellite + data in the NCEP Gridpoint Statistical Interpolation (GSI) system, + especially for surface-sensitive satellite channels. + + Zheng et al.(2009) \cite zheng_et_al_2009 proposed a new formulation on + \f$ln(Z_{0m}^,/Z_{0t})\f$ as follows: +\f[ + ln(Z_{0m}^,/Z_{0t})=(1-GVF)^2C_{zil}k(u*Z_{0g}/\nu)^{0.5} +\f] + where \f$Z_{0m}^,\f$ is the effective momentum roughness length + computed in the following equation for each grid, \f$Z_{0t}\f$ + is the roughness lenghth for heat, \f$C_{zil}\f$ is a coefficient + (taken as 0.8), k is the Von Karman constant (0.4), + \f$\nu=1.5\times10^{-5}m^{2}s^{-1}\f$ is the molecular viscosity, + \f$u*\f$ is the friction velocity, and \f$Z_{0g}\f$ is the bare + soil roughness length for momentum (taken as 0.01). + \n In order to consider the convergence of \f$Z_{0m}\f$ between + fully vegetated and bare soil, the effective \f$Z_{0m}^,\f$ is + computed: +\f[ + \ln(Z_{0m}^,)=(1-GVF)^{2}\ln(Z_{0g})+\left[1-(1-GVF)^{2}\right]\ln(Z_{0m}) +\f] + +\image html roughness_length_fig1.png "Figure 1: Comparison of LST simulated in GFS and verification with the observations. (a) Difference between GFS and GOES in the control run at 18:00 UTC; (b) Difference between GFS and GOES with the new formulation run at 18:00 UTC, averaged from 1 to 3 July 2007" width=10cm + + Figure 1 show the 3 day average land surface skin temperature predicted + by the GFS and comparison with the GOES-derived satellite measurements. + At 18:00 UTC (midday in local time over the central United States) in + the control run (Figure 1a), a substantial cold bias can be found over + the west half of CONUS (i.e., arid or semiarid regions). The new roughness + length formulations significantly reduce the cold bias in the western + CONUS, while the LST in the eastern CONUS, where the bias is small in + the control run, is not much affected. + +\image html roughness_length_fig2.png "Fiure 2: Average diurnal cycle on 1-3 July 2007 for verification of LST with GOES (black) and SURFRAD (blue) at Desert Rock, Nevada; red and green lines are for the control and sensitivity runs, respectively" width=10cm + + The Desert Rock station (\f$36.63^oN\f$, \f$116.02^oW\f$), located in the Nevada + desert,is one of the observation stations within the SURFRAD network. + The GOES-derived LST is very similar to the SURFRAD obervations (Figure 2). + However, the old GFS run produces very low LST, compared to the observations, + especially during daytime. During midday, the cold bias can reach up to + \f$-15^oC\f$. The new formulation run produces a reasonable LST diurnal cycle. + The daytime LST increases substantially and is very close to the observations. + +\section intra_rough 2. Intraphysics Communication +\ref arg_table_sfc_ex_coef_run + +\section gen_rough 3. General Algorithm + + + +*/ diff --git a/physics/docs/txt/GFS_SFCSICE.txt b/physics/docs/txt/GFS_SFCSICE.txt new file mode 100644 index 000000000..ad71d7cb1 --- /dev/null +++ b/physics/docs/txt/GFS_SFCSICE.txt @@ -0,0 +1,58 @@ +/** +\page GFS_SFCSICE GFS Three-Layer Thermodynamics Sea Ice Scheme +\section des_sice 1. Description + This is three-layer thermodynomics sea-ice model based on Winton (2000) \cite winton_2000. + + Sea ice is a thin skin of frozen water covering the polar oceans. The sea ice strongly + interacts with both the atmosphere above and the ocean underneath in the high + latitudes. In a coupled weather/climate system, changes in sea ice extent, thickness and concentration + regionally or globally would influence oceanic and atmospheric conditions, which in turn affect the + sea ice distribution. The physical and dynamical processes affecting the weather and climate are + considered as follows. + + The high albedo of the sea ice reflects more solar radiation back to the space. The feedbacks are + considered as positive. The broader the sea ice cover, the higher the surface albedo, which result + in less amount of solar radiation absorbed at the Earth's surface. A cooler surface would favor more + sea ice to form. The process would be reversed in less sea ice situation. + + The sea ice restricts the heat/water exchange between the air and ocean. The presence of extensive + areas of sea ice would suppress the heat loss in winter and the heat gain in summer by the ocean. + Even a thin ice cover influences the turbulent heat transfer significantly between ocean and + atmosphere. The surface fluxes of sensible and latent heat can be greater by up to two orders of magnitude + at the open water surface of a lead or polynya than that through (snow covered) pack ice. + + The sea ice modifies air/sea momentum transfer, ocean fresh water balance and ocean circulation. + The freezing and melting of the ocean surface and the associated fluxes of salt and heat produce major + changes in the density structure of the polar water. Formation of sea ice injects salt into the ocean + makes the water heavier and more convectively unstable, conversely when melting occurs, stable and fresh + layers can prevent deep covective activity. + + A sea ice model, in general, may contain subcomponents treating 1)dynamics (ice motion), + 2)ice transport, 3) multiple ice thickness categories (including leads), 4) surface albedo, + and 5) vertical thermodynamics. GFS sea ice scheme is concerned with a scheme for the + last of these processes. + + A three-layer thermodynamic sea ice model has been coupled to NCEP GFS. It predicts sea ice/snow thickness, + the surface temperature and ice temperature structure. In each model grid box, the heat and moisture + fluxes and albedo are treated separately for the ice and the open water. + + \image html GFS_sice_wonton2000_fig1.png "Fig.1 Schematic representation of the three-layer model" width=5cm + The model has four prognostic variables: the snow layer thickness \f$h_s\f$, the ice layer thickness + \f$h_i\f$, the upper and lower ice layer temperatures located at the midpoints of the layers + \f$h_i/4\f$ and \f$3h_i/4\f$ below the ice surface, respectively \f$T_1\f$ and \f$T_2\f$. The temperature of + the bottom of the ice is fixed at \f$T_f\f$, the freezing temperature of seawater. The temperature of + the top of the ice or snow, \f$T_s\f$, is determined from the surface energy balance. + + The model consists of a zero-heat-capacity snow layer overlying two equally thick sea ice layers (Fig.1). + The upper ice layer has a variable heat capacity to represent brine pockets. + +\image html schematic_sice.png "Fig.2 NCEP Sea Ice Model System Diagram" width=10cm + +\section intra_sice 2. Intraphysics Communication +\ref arg_table_sfc_sice_run + +\section gen_sice 3. General Algorithm + + + +*/ diff --git a/physics/docs/txt/GFS_ZHAOC.txt b/physics/docs/txt/GFS_ZHAOC.txt new file mode 100644 index 000000000..1943c671e --- /dev/null +++ b/physics/docs/txt/GFS_ZHAOC.txt @@ -0,0 +1,70 @@ +/** +\page GFS_ZHAOC GFS Zhao-Carr Microphysics Scheme +\section des_zhao 1. Description + The GFS scheme for large-scale condensation and precipitation + , based on Zhao and Carr (1997) \cite zhao_and_carr_1997 + and Sundqvist et al. (1989) \cite sundqvist_et_al_1989 . + \image html schematic_MPS.png "Figure 1: Schematic illustration of the precipitation scheme" width=10cm + \details Figure 1 shows a schematic illustration of this scheme. + There are two sources of prognostic cloud condensate, convective + detrainment (see convection) and grid-sale + condensate. The sinks of cloud condensate are grid-scale + precipitation and evaporation of the cloud condensate. Evaporation + of rain in the unsaturated layers below the level of condensation + is also taken into account. All precipitation that penetrates the + lowest atmospheric layer is allowed to fall to the surface. + Subsequent to the May 2001 implementation, excessive amounts of + light precipitation were noted. This was addressed through a minor + implementation in August 2001, which involved a slight modification + of the autoconversion rate of ice. At the same time, an + empirically-based calculation of the effective radius for ice + crystals (Heymsfield and McFarquhar 1996 + \cite heymsfield_and_mcfarquhar_1996) was introduced. + +\section intro_zhao 2. Intraphysics Communication + +\section Gen_zhao 3. General Algorithm + -# For precipitation process: + The parameterization of precipitation is required in order to remove + water from the atmosphere and transport it to the ground. In the + scheme discussed here, simplifications in the precipitation + parameterization are used due to computational limitations required + by operational NWP models. First, consideration of particle size and + shape can be avoided by using the bulk parameterization method + introduced by Kessler (1969) \cite kessler_1969. Second, only two + types of precipitation, rain and snow, are considered in this + scheme. Third, only the most important microphysical processes + associated with the formation of rain and snow are included. + Figure 2 presents the microphysical processes considered in the + precipitation parameterization. + \image html precpd-micop.png "Figure 2: Microphysical processes simulated in the precipitation scheme " width=5cm + Basically, there are four types of microphysical processes + considered here: + - production of rain from cloud water + (\f$P_{racw}\f$, \f$P_{raut}\f$, \f$P_{sacw}\f$) + - production of snow from cloud ice + (\f$P_{saut}\f$, \f$P_{saci}\f$) + - melting of snow to form rain below the freezing level + (\f$P_{sm1}\f$, \f$P_{sm2}\f$) + - the evaporation of precipitation + (\f$E_{rr}\f$, \f$E_{rs}\f$) + + The following two equations can be used to calculate the + precipitation rates of rain and snow at each module level: +\f[ + P_{r}(\eta)=\frac{p_{s}-p_{t}}{g\eta_{s}}\int_{\eta}^{\eta_{t}}(P_{raut}+P_{racw}+P_{sacw}+P_{sm1}+P_{sm2}-E_{rr})d\eta +\f] + and +\f[ + P_{s}(\eta)=\frac{p_{s}-p_{t}}{g\eta_{s}}\int_{\eta}^{\eta_{t}}(P_{saut}+P_{saci}-P_{sm1}-P_{sm2}-E_{rs})d\eta +\f] + where \f$p_{s}\f$ and\f$p_{t}\f$ are the surface pressure and the + pressure at the top of model domain, respectively, and \f$g\f$ is + gravity. The implementation of the precipitation scheme also + includes a simplified procedure of computing \f$P_{r}\f$ + and \f$P_{s}\f$ (Zhao and Carr(1997) \cite zhao_and_carr_1997). + + + + +*/ diff --git a/physics/docs/txt/mainpage.txt b/physics/docs/txt/mainpage.txt index 6fe8bb976..28a416a89 100644 --- a/physics/docs/txt/mainpage.txt +++ b/physics/docs/txt/mainpage.txt @@ -1,48 +1,37 @@ /** -\mainpage 2017 GFS Operational Physics - -\section updates 2017 GFS Physics Upgrades -Effective on Wednesday July 19, 2017, beginning with the 1200 UTC run, NCEP has upgraded the GFS physics as follows: - - Implement Near Surface Sea Temperature (NSST) to replace Real-Time Global SST (RTGSST) to provide more realistic ocean boundary conditions - - Changes to cumulus convection - - Scale-aware, aerosol-aware - - Rain conversion rate decreases with decreasing air temperature above freezing level - - Convective adjustment time in deep convection proportional to convective turn-over time with CAPE approaching zero after adjustment time - - Cloud base mass flux in shallow convection as a function of mean updraft velocity - - Convection trigger condition to suppress the unrealistic summertime spotty precipitation over high mountains - - Convective cloudiness enhanced by suspended cloud condensate in updraft - - A 50% reduction in Rayleigh damping in the upper stratosphere above 2 hPa that improves stratospheric fields - - Land surface changes: - - IGBP 20-type 1-km land classification - - STASGO 19-type 1-km soil classification - - MODIS-based snow free albedo - - MODIS-based maximum snow albedo - - Diurnal albedo treatment - - Unify snow cover, albedo between radiation and land surface model - - Increase ground heat flux under deep snow - - Upgrade surface layer parameterization scheme to modify the roughness-length formulation and introduce a stability parameter constraint in the Monin-Obukhov similarity theory to prevent the land-atmosphere system from fully decoupling leading to excessive cooling of 2m temperature during sunset - -Changes in the land surface and stability parameter should reduce a near surface wintertime cold bias, a rapid temperature drop during sunset and reduce a blockiness apparent in some near-surface fields. Some nighttime warm biases were introduced. Changes in convection should reduce a positive bias in light amounts of precipitation and unrealistic summertime spotty precipitation over high mountains and increase skill in forecasting precipitation. NSST is expected to improve tropical forecasts and may affect mid-latitude oceanic storms. Reducing Rayleigh damping improved wind and temperature forecast in the upper stratosphere. - -Details on the changes and evaluation of the changes of the entire Global Forecast System can be found at: -\n http://www.emc.ncep.noaa.gov/gmb/noor/GFS2017/GFS2017.htm - -\section schemes CCPP Physics Documentation -Please check DTC website https://dtcenter.org/community-code/ipd-ccpp for GMTB IPD/CCPP infrastructure and governance information. -\n The documentation found here corresponds to the state of the operational GFS physics suite as of 2017. Documentation for the operational physics suite can be access through these links: - - \ref RRTMG - - \ref SAMF - - \ref SAMF_shal - - \ref HEDMF - - \ref Zhao-Carr - - \ref Sfc_ex_cal - - \ref GFS_Ice - - \ref NOAH - - \ref GFS_NSST - - \ref GFS_ogwd - - \ref GFS_rayleigh - - \ref GFS_cgwd - - \ref GFS_ozn - - \ref CALPRECIPTYPE +\mainpage Introduction + + +\anchor mainpage-top + +Welcome to the GMTB Common Community Physics Package (CCPP) documentation for \b the \b 2017 \b Operational \b GFS \b physics \b suite. In this website you will find documentation on various aspects of the 2017 operational GFS physics, including basic description, input/output augument list and general/detailed algorithm. + +\author Global Model Test Bed (GMTB) at DTC and NOAA/ESRL + +\copyright GMTB + +Documentation for the individual physics scheme can be access through links in the table: + + +
    GMTB CCPP Documentation
    CCPP Physics Suite Physics Scheme +
    2017 Operational GFS Physics Suite @ref GFS_RRTMG +
    @ref GFS_SAMFdeep +
    @ref GFS_SAMFshal +
    @ref GFS_HEDMF +
    @ref GFS_ZHAOC +
    @ref GFS_SFCLYR +
    @ref GFS_SFCSICE +
    @ref GFS_NOAH +
    @ref GFS_NSST +
    @ref GFS_GWDPS +
    @ref GFS_GWDC +
    @ref GFS_OZPHYS +
    @ref GFS_CALPRECIPTYPE +
    + + You can find more information about +GMTB Interoperable Physics Driver/Common Community Physics Package(IPD/CCPP) on DTC website + + */ diff --git a/physics/docs/txt/mainpage.txt.ORIG b/physics/docs/txt/mainpage.txt.ORIG new file mode 100644 index 000000000..6fe8bb976 --- /dev/null +++ b/physics/docs/txt/mainpage.txt.ORIG @@ -0,0 +1,48 @@ +/** +\mainpage 2017 GFS Operational Physics + +\section updates 2017 GFS Physics Upgrades +Effective on Wednesday July 19, 2017, beginning with the 1200 UTC run, NCEP has upgraded the GFS physics as follows: + - Implement Near Surface Sea Temperature (NSST) to replace Real-Time Global SST (RTGSST) to provide more realistic ocean boundary conditions + - Changes to cumulus convection + - Scale-aware, aerosol-aware + - Rain conversion rate decreases with decreasing air temperature above freezing level + - Convective adjustment time in deep convection proportional to convective turn-over time with CAPE approaching zero after adjustment time + - Cloud base mass flux in shallow convection as a function of mean updraft velocity + - Convection trigger condition to suppress the unrealistic summertime spotty precipitation over high mountains + - Convective cloudiness enhanced by suspended cloud condensate in updraft + - A 50% reduction in Rayleigh damping in the upper stratosphere above 2 hPa that improves stratospheric fields + - Land surface changes: + - IGBP 20-type 1-km land classification + - STASGO 19-type 1-km soil classification + - MODIS-based snow free albedo + - MODIS-based maximum snow albedo + - Diurnal albedo treatment + - Unify snow cover, albedo between radiation and land surface model + - Increase ground heat flux under deep snow + - Upgrade surface layer parameterization scheme to modify the roughness-length formulation and introduce a stability parameter constraint in the Monin-Obukhov similarity theory to prevent the land-atmosphere system from fully decoupling leading to excessive cooling of 2m temperature during sunset + +Changes in the land surface and stability parameter should reduce a near surface wintertime cold bias, a rapid temperature drop during sunset and reduce a blockiness apparent in some near-surface fields. Some nighttime warm biases were introduced. Changes in convection should reduce a positive bias in light amounts of precipitation and unrealistic summertime spotty precipitation over high mountains and increase skill in forecasting precipitation. NSST is expected to improve tropical forecasts and may affect mid-latitude oceanic storms. Reducing Rayleigh damping improved wind and temperature forecast in the upper stratosphere. + +Details on the changes and evaluation of the changes of the entire Global Forecast System can be found at: +\n http://www.emc.ncep.noaa.gov/gmb/noor/GFS2017/GFS2017.htm + +\section schemes CCPP Physics Documentation +Please check DTC website https://dtcenter.org/community-code/ipd-ccpp for GMTB IPD/CCPP infrastructure and governance information. +\n The documentation found here corresponds to the state of the operational GFS physics suite as of 2017. Documentation for the operational physics suite can be access through these links: + - \ref RRTMG + - \ref SAMF + - \ref SAMF_shal + - \ref HEDMF + - \ref Zhao-Carr + - \ref Sfc_ex_cal + - \ref GFS_Ice + - \ref NOAH + - \ref GFS_NSST + - \ref GFS_ogwd + - \ref GFS_rayleigh + - \ref GFS_cgwd + - \ref GFS_ozn + - \ref CALPRECIPTYPE + +*/ diff --git a/physics/docs/txt/mainpage_bootstrapped.txt b/physics/docs/txt/mainpage_bootstrapped.txt new file mode 100644 index 000000000..5667dcb4d --- /dev/null +++ b/physics/docs/txt/mainpage_bootstrapped.txt @@ -0,0 +1,33 @@ +/** +\mainpage Introduction + + +\anchor mainpage-top + +Welcome to the GMTB Common Community Physics Package (CCPP) documentation for \b the \b 2017 \b Operational \b GFS \b physics \b suite. In this website you will find documentation on various aspects of the 2017 operational GFS physics, including basic description, input/output augument list and general/detailed algorithm. + +\author Global Model Test Bed (GMTB) at DTC and NOAA/ESRL + +\copyright GMTB + +Documentation for the individual physics scheme can of 2017 operational GFS physics suite be access through the following links: + + @ref GFS_RRTMG + + @ref GFS_SAMFdeep + + @ref GFS_SAMFshal + + @ref GFS_HEDMF + + @ref GFS_ZHAOC + + @ref GFS_SFCLYR + + @ref GFS_SFCSICE + + @ref GFS_NOAH + + @ref GFS_NSST + + @ref GFS_GWDPS + + @ref GFS_GWDC + + @ref GFS_OZPHYS + + @ref GFS_CALPRECIPTYPE + + You can find more information about +GMTB Interoperable Physics Driver/Common Community Physics Package(IPD/CCPP) on DTC website + + + +*/ diff --git a/physics/gwdps.f b/physics/gwdps.f index 232962539..3659929a6 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -279,6 +279,7 @@ end subroutine gwdps_init !! | ipr | horizontal_index_of_printed_column | horizontal index of column used in debugging printouts | index | 0 | integer | default | in | F | !! !> \section gen_gwdps General Algorithm +!> \section det_gwdps Detailed Algorithm !> @{ subroutine gwdps_run( & & IM,IX,IY,KM,A,B,C,U1,V1,T1,Q1,KPBL, & diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 4ec32240c..4574fc8b4 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -158,7 +158,7 @@ end subroutine sasasdeep_finalize !! -# For the "feedback control", calculate updated values of the state !! variables by multiplying the cloud base mass flux and the tendencies !! calculated per unit cloud base mass flux from the static control. -!! \section detailed Detailed Algorithm +!! \section detailed_deep Detailed Algorithm !! @{ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & & ql2,q1,t1,u1,v1,cldwrk,rn,kbot,ktop,kcnv,islimsk,garea, & diff --git a/physics/radsw_main.f b/physics/radsw_main.f index 66e617635..858d2a627 100644 --- a/physics/radsw_main.f +++ b/physics/radsw_main.f @@ -564,7 +564,7 @@ end subroutine swrad_init !! | cld_ssa | cloud_single_scattering_albedo | cloud single scattering albedo | frac | 2 | real | kind_phys | in | T | !! | cld_asy | cloud_asymmetry_parameter | cloud asymmetry parameter | none | 2 | real | kind_phys | in | T | !! -!> \section General_swrad General Algorithm +!> \section gen_swrad General Algorithm !> @{ !----------------------------------- subroutine swrad_run & diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index 13450e793..3f07e197f 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -848,7 +848,6 @@ end subroutine sfc_nst_post_finalize !! ! \section NSST_general_algorithm General Algorithm ! -! Blah blah general algorithm ! ! \section NSST_detailed_algorithm Detailed Algorithm ! @{ diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index c57fb7298..6c8ae0fb0 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -69,7 +69,7 @@ end subroutine sfc_sice_finalize !>\defgroup gfs_sice_main GFS sfc_sice Main !! @{ !! \ingroup GFS_Ice -!! \section arg_table_sfc_sice_run Arguments +!! \section arg_table_sfc_sice_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------------|-----------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | From a1bf4da3df69c6592c1840abcd485fd541b212ad Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Mon, 12 Feb 2018 16:57:19 -0700 Subject: [PATCH 14/22] a few fix was done. --- physics/docs/ccpp_dox | 15 +-- physics/docs/{ccpp_dox_Feb08 => ccpp_dox_bts} | 19 ++-- physics/docs/img/GFS_zhaocarr_schematic.png | Bin 0 -> 38829 bytes physics/docs/img/schematic_MPS.png | Bin 122136 -> 0 bytes physics/docs/txt/GFS_RAYLEIGH.txt | 17 +++ physics/docs/txt/GFS_ZHAOC.txt | 102 ++++++++++-------- physics/docs/txt/mainpage_bootstrapped.txt | 1 + physics/gscond.f | 56 ++-------- physics/gwdc.f | 4 +- physics/gwdps.f | 4 +- physics/mfshalcnv.f | 4 +- physics/ozphys.f | 6 +- physics/precpd.f | 53 ++------- physics/sfc_sice.f | 4 +- 14 files changed, 122 insertions(+), 163 deletions(-) rename physics/docs/{ccpp_dox_Feb08 => ccpp_dox_bts} (95%) create mode 100644 physics/docs/img/GFS_zhaocarr_schematic.png delete mode 100644 physics/docs/img/schematic_MPS.png create mode 100644 physics/docs/txt/GFS_RAYLEIGH.txt diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index add5d2a85..1c92b257e 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -1,6 +1,6 @@ # Doxyfile 1.8.11 DOXYFILE_ENCODING = UTF-8 -PROJECT_NAME = "GMTB Common Community Physics Package (CCPP) Documentation" +PROJECT_NAME = "GMTB Common Community Physics Package(CCPP) Documentation" PROJECT_NUMBER = "Version 0" PROJECT_BRIEF = "" PROJECT_LOGO = img/dtc_logo.png @@ -89,7 +89,7 @@ SHOW_USED_FILES = YES SHOW_FILES = YES SHOW_NAMESPACES = YES FILE_VERSION_FILTER = -LAYOUT_FILE = +LAYOUT_FILE = ccpp_dox_layout.xml CITE_BIB_FILES = library.bib QUIET = NO WARNINGS = YES @@ -113,6 +113,7 @@ INPUT = txt/mainpage_bootstrapped.txt \ txt/GFS_GWDC.txt \ txt/GFS_OZPHYS.txt \ txt/GFS_CALPRECIPTYPE.txt \ + txt/GFS_RAYLEIGH.txt \ ### Radiation ../radiation_aerosols.f \ ../radiation_astronomy.f \ @@ -190,11 +191,11 @@ IGNORE_PREFIX = GENERATE_HTML = YES HTML_OUTPUT = html HTML_FILE_EXTENSION = .html -HTML_HEADER = ./bootstrapped/header.html -HTML_FOOTER = ./bootstrapped/footer.html +HTML_HEADER = +HTML_FOOTER = HTML_STYLESHEET = -HTML_EXTRA_STYLESHEET = ./bootstrapped/customdoxygen.css -HTML_EXTRA_FILES = ./bootstrapped/doxy-boot.js +HTML_EXTRA_STYLESHEET = ccpp_dox_extra_style.css +HTML_EXTRA_FILES = HTML_COLORSTYLE_HUE = 220 HTML_COLORSTYLE_SAT = 100 HTML_COLORSTYLE_GAMMA = 80 @@ -224,7 +225,7 @@ QHG_LOCATION = GENERATE_ECLIPSEHELP = NO ECLIPSE_DOC_ID = org.doxygen.Project DISABLE_INDEX = YES -GENERATE_TREEVIEW = NO +GENERATE_TREEVIEW = YES ENUM_VALUES_PER_LINE = 4 TREEVIEW_WIDTH = 250 EXT_LINKS_IN_WINDOW = NO diff --git a/physics/docs/ccpp_dox_Feb08 b/physics/docs/ccpp_dox_bts similarity index 95% rename from physics/docs/ccpp_dox_Feb08 rename to physics/docs/ccpp_dox_bts index 4963cfbc5..3efd05c67 100644 --- a/physics/docs/ccpp_dox_Feb08 +++ b/physics/docs/ccpp_dox_bts @@ -1,7 +1,7 @@ # Doxyfile 1.8.11 DOXYFILE_ENCODING = UTF-8 -PROJECT_NAME = "GMTB CCPP Documentation" -PROJECT_NUMBER = "V0" +PROJECT_NAME = "GMTB Common Community Physics Package (CCPP) Documentation" +PROJECT_NUMBER = "Version 0" PROJECT_BRIEF = "" PROJECT_LOGO = img/dtc_logo.png OUTPUT_DIRECTORY = doc @@ -89,7 +89,7 @@ SHOW_USED_FILES = YES SHOW_FILES = YES SHOW_NAMESPACES = YES FILE_VERSION_FILTER = -LAYOUT_FILE = ccpp_dox_layout.xml +LAYOUT_FILE = CITE_BIB_FILES = library.bib QUIET = NO WARNINGS = YES @@ -99,7 +99,7 @@ WARN_NO_PARAMDOC = NO WARN_AS_ERROR = NO WARN_FORMAT = WARN_LOGFILE = -INPUT = txt/mainpage.txt \ +INPUT = txt/mainpage_bootstrapped.txt \ txt/GFS_RRTMG.txt \ txt/GFS_SAMFdeep.txt \ txt/GFS_SAMFshal.txt \ @@ -113,6 +113,7 @@ INPUT = txt/mainpage.txt \ txt/GFS_GWDC.txt \ txt/GFS_OZPHYS.txt \ txt/GFS_CALPRECIPTYPE.txt \ + txt/GFS_RAYLEIGH.txt \ ### Radiation ../radiation_aerosols.f \ ../radiation_astronomy.f \ @@ -190,11 +191,11 @@ IGNORE_PREFIX = GENERATE_HTML = YES HTML_OUTPUT = html HTML_FILE_EXTENSION = .html -HTML_HEADER = -HTML_FOOTER = +HTML_HEADER = ./bootstrapped/header.html +HTML_FOOTER = ./bootstrapped/footer.html HTML_STYLESHEET = -HTML_EXTRA_STYLESHEET = ccpp_dox_extra_style.css 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Description +This is the Rayleigh friction calculation with total energy conservation. +\n Role of Rayleigh friction, it attempts to resolve two issues: + - The top lid model effects, sponge layer to suppress resolved wave reflections and extra-heating + - The winter-summer zonal wind drag in the strato-mesosphere + +\section intra_rayleigh 2. Intraphysics Communication +\sa \ref arg_table_rayleigh_damp_run + +\section gen_ozone 3. General Algorithm + + + + +*/ diff --git a/physics/docs/txt/GFS_ZHAOC.txt b/physics/docs/txt/GFS_ZHAOC.txt index 1943c671e..1682d2ced 100644 --- a/physics/docs/txt/GFS_ZHAOC.txt +++ b/physics/docs/txt/GFS_ZHAOC.txt @@ -1,53 +1,33 @@ /** \page GFS_ZHAOC GFS Zhao-Carr Microphysics Scheme \section des_zhao 1. Description - The GFS scheme for large-scale condensation and precipitation - , based on Zhao and Carr (1997) \cite zhao_and_carr_1997 - and Sundqvist et al. (1989) \cite sundqvist_et_al_1989 . - \image html schematic_MPS.png "Figure 1: Schematic illustration of the precipitation scheme" width=10cm - \details Figure 1 shows a schematic illustration of this scheme. - There are two sources of prognostic cloud condensate, convective - detrainment (see convection) and grid-sale - condensate. The sinks of cloud condensate are grid-scale - precipitation and evaporation of the cloud condensate. Evaporation - of rain in the unsaturated layers below the level of condensation - is also taken into account. All precipitation that penetrates the - lowest atmospheric layer is allowed to fall to the surface. - Subsequent to the May 2001 implementation, excessive amounts of - light precipitation were noted. This was addressed through a minor - implementation in August 2001, which involved a slight modification - of the autoconversion rate of ice. At the same time, an - empirically-based calculation of the effective radius for ice - crystals (Heymsfield and McFarquhar 1996 - \cite heymsfield_and_mcfarquhar_1996) was introduced. + This is the GFS scheme for large-scale condensation and precipitation which is based on + Zhao and Carr (1997) \cite zhao_and_carr_1997 and Sundqvist et al.(1989) \cite sundqvist_et_al_1989 . + The main feature of this parameterization is the inclusion of cloud water and cloud ice in both the + convective and grid-scale precipitation paramterizations, and use only one predictive variable, the + cloud water/ice mixing ratio \f$m\f$, to represent both cloud water and cloud ice. This will reduce + the model computation time and storage requirements. -\section intro_zhao 2. Intraphysics Communication + Figure 1 shows a schematic illustration of this scheme. + There are two sources of prognostic cloud condensate, namely convective + detrainment (sasasdeep_run() and sasasshal_run()) and grid-sale condensation (gscond_run()). + Both of them produce either cloud water or cloud ice, depending on + the cloud substance at and above the grid point at current and previous time steps, and on the temperature. Evaporation of + cloud is allowed at points where the relative humidity is lower than the critical value required for condensation. Precipitation + is diagnostically calculated directly from the cloud water/ice mixing ratio. Both frozen and liquid precipitation can be + prognostically produced, enabling this scheme to predict precipitation type. + + \image html GFS_zhaocarr_schematic.png "Figure 1: Schematic illustration of the precipitation scheme" width=10cm -\section Gen_zhao 3. General Algorithm - -# For precipitation process: The parameterization of precipitation is required in order to remove - water from the atmosphere and transport it to the ground. In the - scheme discussed here, simplifications in the precipitation - parameterization are used due to computational limitations required - by operational NWP models. First, consideration of particle size and - shape can be avoided by using the bulk parameterization method - introduced by Kessler (1969) \cite kessler_1969. Second, only two - types of precipitation, rain and snow, are considered in this - scheme. Third, only the most important microphysical processes - associated with the formation of rain and snow are included. - Figure 2 presents the microphysical processes considered in the - precipitation parameterization. - \image html precpd-micop.png "Figure 2: Microphysical processes simulated in the precipitation scheme " width=5cm - Basically, there are four types of microphysical processes - considered here: - - production of rain from cloud water - (\f$P_{racw}\f$, \f$P_{raut}\f$, \f$P_{sacw}\f$) - - production of snow from cloud ice - (\f$P_{saut}\f$, \f$P_{saci}\f$) - - melting of snow to form rain below the freezing level - (\f$P_{sm1}\f$, \f$P_{sm2}\f$) - - the evaporation of precipitation - (\f$E_{rr}\f$, \f$E_{rs}\f$) + water from the atmosphere and transport it to the ground. + For the precipitation production, only the principle microphysical processes associated with formation of rain and + snow are inlcuded. Figure 2 presents the microphysical processes considered in the microphysics scheme. Basically, + there are four types of microphysical processes considered here: + + Production of rain from cloud water (\f$P_{racw}\f$, \f$P_{raut}\f$, \f$P_{sacw}\f$) + + Production of snow from cloud ice (\f$P_{saut}\f$, \f$P_{saci}\f$) + + Melting of snow to form rain below the freezing level (\f$P_{sm1}\f$, \f$P_{sm2}\f$) + + Evaporation of precipitation (\f$E_{rr}\f$, \f$E_{rs}\f$) The following two equations can be used to calculate the precipitation rates of rain and snow at each module level: @@ -64,6 +44,40 @@ includes a simplified procedure of computing \f$P_{r}\f$ and \f$P_{s}\f$ (Zhao and Carr(1997) \cite zhao_and_carr_1997). +\image html precpd-micop.png "Figure 2: Microphysical processes simulated in the precipitation scheme " width=10cm + + Some processes, such as the freezing of raindrops and the interaction between rain drops and cloud ice, have been ignored + since the upward motion on the synoptic scale is too weak to advect the raindrops upward. Additionally, precipitation is + diagnostically calculated directly from the cloud mixing ratio. + + + Subsequent to the May 2001 implementation, excessive amounts of + light precipitation were noted. This was addressed through a minor + implementation in August 2001, which involved a slight modification + of the autoconversion rate of ice. At the same time, an + empirically-based calculation of the effective radius for ice + crystals (Heymsfield and McFarquhar 1996 + \cite heymsfield_and_mcfarquhar_1996) was introduced. + +\section intro_zhao 2. Intraphysics Communication + + For grid-scale condensation and evaporation of cloud process + \sa \ref arg_table_gscond_run + + For precipitation (snow or rain) production + \sa \ref arg_table_precpd_run + +\section Gen_zhao 3. General Algorithm + + For grid-scale condensation and evaporation of cloud process + \sa \ref general_gscond + + For precipitation (snow or rain) production + \sa \ref general_precpd + +\section det_zhao 4. Detailed Algorithm + + For grid-scale condensation and evaporation of cloud process + \sa \ref Zhao-Carr_cond_detailed + + For precipitation (snow or rain) production + \sa \ref Zhao-Carr_precip_detailed + + diff --git a/physics/docs/txt/mainpage_bootstrapped.txt b/physics/docs/txt/mainpage_bootstrapped.txt index 5667dcb4d..129e42b99 100644 --- a/physics/docs/txt/mainpage_bootstrapped.txt +++ b/physics/docs/txt/mainpage_bootstrapped.txt @@ -24,6 +24,7 @@ Documentation for the individual physics scheme can of 2017 operational GFS phys + @ref GFS_GWDC + @ref GFS_OZPHYS + @ref GFS_CALPRECIPTYPE + + @ref GFS_RAYLEIGH You can find more information about GMTB Interoperable Physics Driver/Common Community Physics Package(IPD/CCPP) on DTC website diff --git a/physics/gscond.f b/physics/gscond.f index 1e5013d07..556245bf9 100644 --- a/physics/gscond.f +++ b/physics/gscond.f @@ -8,38 +8,7 @@ module GFS_zhaocarr_gscond !> \defgroup Zhao-Carr GFS Zhao-Carr Microphysics !! @{ -!! \brief The GFS scheme for large-scale condensation and precipitation -!! , based on Zhao and Carr (1997) \cite zhao_and_carr_1997 -!! and Sundqvist et al. (1989) \cite sundqvist_et_al_1989 . -!! \image html schematic_MPS.png "Figure 1: Schematic illustration of the precipitation scheme" width=10cm -!! \details Figure 1 shows a schematic illustration of this scheme. -!! There are two sources of prognostic cloud condensate, convective -!! detrainment (see convection) and grid-sale -!! condensate. The sinks of cloud condensate are grid-scale -!! precipitation and evaporation of the cloud condensate. Evaporation -!! of rain in the unsaturated layers below the level of condensation -!! is also taken into account. All precipitation that penetrates the -!! lowest atmospheric layer is allowed to fall to the surface. -!! Subsequent to the May 2001 implementation, excessive amounts of -!! light precipitation were noted. This was addressed through a minor -!! implementation in August 2001, which involved a slight modification -!! of the autoconversion rate of ice. At the same time, an -!! empirically-based calculation of the effective radius for ice -!! crystals (Heymsfield and McFarquhar 1996 -!! \cite heymsfield_and_mcfarquhar_1996) was introduced. -!> \section tune Important Tunable Parameters -!! The parameters below, which can be set through a namelist, influence -!! the amount of cloud condensate in the atmosphere and thus the cloud -!! radiative properties: -!! - PSAUTCO, PRAUTCO: Auto conversion coefficients (ice and water) -!! - WMINCO(2): Coefficients for minimum value of cloud condensate to -!! conversion from condensate (water and ice) to precipitation -!! - EVPCO: Coefficient for evaporation of precipitation !! -!! \section intraphysics_gscond Intraphysics Communication -!! -!> \defgroup condense Grid-Scale Condensation and Evaporation of Cloud -!! @{ ! \brief Brief description of the subroutine ! @@ -48,18 +17,11 @@ module GFS_zhaocarr_gscond subroutine gscond_init end subroutine gscond_init - -!> \defgroup gfs_gscond GFS gscond Main +!> \defgroup condense Grid-Scale Condensation and Evaporation of Cloud +!! @{ !! \brief This subroutine computes grid-scale condensation and evaporation of !! cloud condensate. !! -!! There are two sources of condensation, one from large-scale -!! processes and the other from convective processes. Both of them -!! produce either cloud water or cloud ice, depending on the cloud -!! substance at and above the grid point at current and previous time -!! steps, and on the temperature. Evaporation of cloud is allowed at -!! points where the relative humidity is lower than the critical value -!! required for condensation. !! \section arg_table_gscond_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------|----------------------------------------------------------|---------|------|---------|-----------|--------|----------| @@ -85,9 +47,13 @@ end subroutine gscond_init !! | lprnt | flag_print | flag for printing diagnostics to output | flag | 0 | logical | | in | F | !! | ipr | horizontal_index_of_printed_column | horizontal index of printed column | index | 0 | integer | | in | F | !! -!! \section def Definition of symbols -!! - \f$C_{g}\f$: grid-scale condensation rate (\f$s^{-1}\f$) -!! - \f$E_{c}\f$: evaporation rate of cloud (\f$s^{-1}\f$) +!> \section general_gscond General Algorithm +!! -# Calculate ice-water identification number \f$IW\f$ in order to make a distinction betwee +!! cloud water and cloud ice (table2 in Zhao and Carr (1997)). +!! -# Calculate the changes in \f$t\f$, \f$q\f$ and \f$p\f$ due to all the processes except microphysics. +!! -# Calculate cloud evaporation process (\f$E_c\f$) +!! \todo general_gscond +!!\n Cloud evaporation is allowed to take place only where !> \section Zhao-Carr_cond_detailed Detailed Algorithm !> @{ subroutine gscond_run (im,ix,km,dt,dtf,prsl,ps,q,clw1,clw2 & @@ -495,7 +461,7 @@ subroutine gscond_run (im,ix,km,dt,dtf,prsl,ps,q,clw1,clw2 & enddo ! end of k-loop! ! !********************************************************************* -!> -# End of the condensation/evaporation loop (end of i-loop,k-loop) +!> -# End of the condensation/evaporation loop (end of i-loop,k-loop). !********************************************************************* ! @@ -536,6 +502,7 @@ subroutine gscond_run (im,ix,km,dt,dtf,prsl,ps,q,clw1,clw2 & return end subroutine gscond_run !> @} +!! @} ! \brief Brief description of the subroutine ! @@ -545,7 +512,6 @@ subroutine gscond_finalize end subroutine gscond_finalize -!> @} !! @} end module GFS_zhaocarr_gscond diff --git a/physics/gwdc.f b/physics/gwdc.f index c9f879413..d888e5836 100644 --- a/physics/gwdc.f +++ b/physics/gwdc.f @@ -75,7 +75,7 @@ end subroutine gwdc_pre_init ! \brief Brief description of the subroutine ! -!> \section arg_table_gwdc_pre_run Argument Table +! \section arg_table_gwdc_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|--------------------------------------------------------------------------|---------------------------------------------------------------|-------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -1536,7 +1536,7 @@ end subroutine gwdc_post_init ! \brief Brief description of the subroutine ! -!> \section arg_table_gwdc_post_run Argument Table +! \section arg_table_gwdc_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------------|--------------------------------------------------------------------------|------------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | default | in | F | diff --git a/physics/gwdps.f b/physics/gwdps.f index 3659929a6..557ed6b40 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -112,7 +112,7 @@ end subroutine gwdps_pre_init ! \ingroup GFS_ogwd ! \brief Brief description of the subroutine ! -!> \section arg_table_gwdps_pre_run Argument Table +! \section arg_table_gwdps_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-------------------------------------------------------------------------|------------------------------------------------------------------------------------------|---------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal dimension | count | 0 | integer | default | in | F | @@ -1367,7 +1367,7 @@ end subroutine gwdps_post_init ! \ingroup GFS_ogwd ! \brief Brief description of the subroutine -!> \section arg_table_gwdps_post_run Argument Table +! \section arg_table_gwdps_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-----------------------------------------------------------|------------------------------------------------------------------|-------|------|---------|-----------|--------|----------| !! | lssav | flag_diagnostics | flag for calculating diagnostic fields | flag | 0 | logical | default | in | F | diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 61e6db260..48eb13e42 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -1718,8 +1718,8 @@ end module sasas_shal module sasas_shal_post contains -!> \brief Brief description of the subroutine -!! +! \brief Brief description of the subroutine +! !! \section arg_table_sasasshal_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|----------------------------------------------------------|----------------------------------------------------------------------|---------|------|-------------------------------|-----------|--------|----------| diff --git a/physics/ozphys.f b/physics/ozphys.f index 07188b53b..1c07e04f7 100644 --- a/physics/ozphys.f +++ b/physics/ozphys.f @@ -74,9 +74,9 @@ end subroutine ozphys_init !! !! \section genal_ozphys General Algorithm !> @{ - subroutine ozphys_run ( & - & ix, im, levs, ko3, dt, ozi, ozo, tin, po3, & - & prsl, prdout, pl_coeff, delp, ldiag3d, & + subroutine ozphys_run ( & + & ix, im, levs, ko3, dt, ozi, ozo, tin, po3,& + & prsl, prdout, pl_coeff, delp, ldiag3d,& & ozp, me) ! ! this code assumes that both prsl and po3 are from bottom to top diff --git a/physics/precpd.f b/physics/precpd.f index 2e7d090b2..c2880e4db 100644 --- a/physics/precpd.f +++ b/physics/precpd.f @@ -5,10 +5,6 @@ module GFS_zhaocarr_precpd contains -!> \ingroup Zhao-Carr -!> \defgroup precip Precipitation (snow or rain) Production -!! @{ - ! \brief Brief description of the subroutine ! ! \section arg_table_precpd_init Argument Table @@ -16,8 +12,9 @@ module GFS_zhaocarr_precpd subroutine precpd_init () end subroutine precpd_init - -!> \defgroup gfs_precpd GFS precpd Main +!> \defgroup precip Precipitation (snow or rain) Production +!! \ingroup Zhao-Carr +!! @{ !! \brief This subroutine computes the conversion from condensation to !! precipitation (snow or rain) or evaporation of rain. !! @@ -45,45 +42,8 @@ end subroutine precpd_init !! | lprnt | flag_print | flag for printing diagnostics to output | flag | 0 | logical | | in | F | !! | jpr | horizontal_index_of_printed_column | horizontal index of printed column | index | 0 | integer | | in | F | !! -!! \section general_precpd General Algorithm -!! The parameterization of precipitation is required in order to remove -!! water from the atmosphere and transport it to the ground. In the -!! scheme discussed here, simplifications in the precipitation -!! parameterization are used due to computational limitations required -!! by operational NWP models. First, consideration of particle size and -!! shape can be avoided by using the bulk parameterization method -!! introduced by Kessler (1969) \cite kessler_1969. Second, only two -!! types of precipitation, rain and snow, are considered in this -!! scheme. Third, only the most important microphysical processes -!! associated with the formation of rain and snow are included. -!! Figure 2 presents the microphysical processes considered in the -!! precipitation parameterization. -!! \image html precpd-micop.png "Figure 2: Microphysical processes simulated in the precipitation scheme " width=5cm -!! Basically, there are four types of microphysical processes -!! considered here: -!! - production of rain from cloud water -!! (\f$P_{racw}\f$, \f$P_{raut}\f$, \f$P_{sacw}\f$) -!! - production of snow from cloud ice -!! (\f$P_{saut}\f$, \f$P_{saci}\f$) -!! - melting of snow to form rain below the freezing level -!! (\f$P_{sm1}\f$, \f$P_{sm2}\f$) -!! - the evaporation of precipitation -!! (\f$E_{rr}\f$, \f$E_{rs}\f$) -!! -!! The following two equations can be used to calculate the -!! precipitation rates of rain and snow at each module level: -!!\f[ -!! P_{r}(\eta)=\frac{p_{s}-p_{t}}{g\eta_{s}}\int_{\eta}^{\eta_{t}}(P_{raut}+P_{racw}+P_{sacw}+P_{sm1}+P_{sm2}-E_{rr})d\eta -!!\f] -!! and -!!\f[ -!! P_{s}(\eta)=\frac{p_{s}-p_{t}}{g\eta_{s}}\int_{\eta}^{\eta_{t}}(P_{saut}+P_{saci}-P_{sm1}-P_{sm2}-E_{rs})d\eta -!!\f] -!! where \f$p_{s}\f$ and\f$p_{t}\f$ are the surface pressure and the -!! pressure at the top of model domain, respectively, and \f$g\f$ is -!! gravity. The implementation of the precipitation scheme also -!! includes a simplified procedure of computing \f$P_{r}\f$ -!! and \f$P_{s}\f$ (Zhao and Carr(1997) \cite zhao_and_carr_1997). +!> \section general_precpd General Algorithm +!! \todo general precpd !! \section Zhao-Carr_precip_detailed Detailed Algorithm !! @{ subroutine precpd_run (im,ix,km,dt,del,prsl,q,cwm,t,rn,sr & @@ -737,6 +697,7 @@ subroutine precpd_run (im,ix,km,dt,del,prsl,q,cwm,t,rn,sr & return end subroutine precpd_run !> @} +!> @} ! \brief Brief description of the subroutine ! @@ -745,6 +706,4 @@ end subroutine precpd_run subroutine precpd_finalize end subroutine precpd_finalize -!> @} - end module GFS_zhaocarr_precpd diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 6c8ae0fb0..28c808f5a 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -788,7 +788,7 @@ subroutine sfc_sice_pre_finalize end subroutine sfc_sice_pre_finalize -!> \section arg_table_sfc_sice_pre_run Argument Table +! \section arg_table_sfc_sice_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------------|-------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -855,7 +855,7 @@ end subroutine sfc_sice_post_finalize !! -!> \section arg_table_sfc_sice_post_run Argument Table +! \section arg_table_sfc_sice_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-------------------------------------------------------|---------------------------------------------|---------------|------|---------|-----------|--------|----------| !! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | From f7dad94b8985dfd67544c75b3f9a8436ebbbf25c Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Thu, 15 Feb 2018 10:23:41 -0700 Subject: [PATCH 15/22] multiple fix is done. --- physics/docs/ccpp_dox | 3 + physics/docs/img/GFS_Operational_Physics.png | Bin 252976 -> 0 bytes .../img/GFS_Operational_Physics.png.bak.png | Bin 414866 -> 0 bytes physics/docs/img/Hybrid_EDMF_Flowchart.png | Bin 52018 -> 0 bytes physics/docs/img/SAS_Flowchart.png | Bin 42224 -> 0 bytes physics/docs/img/Shallow_SAS_Flowchart.png | Bin 39492 -> 0 bytes physics/docs/img/precpd-micop.png | Bin 159216 -> 86794 bytes physics/docs/library.bib | 21 ++- physics/docs/txt/GFS_GWDC.txt | 64 ++++----- physics/docs/txt/GFS_GWDPS.txt | 5 +- physics/docs/txt/GFS_NSST.txt | 26 ++-- physics/docs/txt/GFS_SFCLYR.txt | 56 +++----- physics/docs/txt/GFS_SFCSICE.txt | 8 +- physics/docs/txt/GFS_ZHAOC.txt | 2 +- physics/gscond.f | 10 +- physics/gwdc.f | 89 +------------ physics/gwdps.f | 120 +---------------- physics/module_nst_model.f90 | 7 +- physics/module_nst_parameters.f90 | 5 + physics/module_nst_water_prop.f90 | 15 +++ physics/precpd.f | 31 +++-- physics/sfc_diff.f | 122 ++++++------------ physics/sfc_drv.f | 18 +-- physics/sfc_nst.f | 33 +---- physics/sfc_sice.f | 114 +++++++--------- 25 files changed, 250 insertions(+), 499 deletions(-) delete mode 100644 physics/docs/img/GFS_Operational_Physics.png delete mode 100644 physics/docs/img/GFS_Operational_Physics.png.bak.png delete mode 100644 physics/docs/img/Hybrid_EDMF_Flowchart.png delete mode 100644 physics/docs/img/SAS_Flowchart.png delete mode 100644 physics/docs/img/Shallow_SAS_Flowchart.png diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index 1c92b257e..b0a5f8b2a 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -149,6 +149,9 @@ INPUT = txt/mainpage_bootstrapped.txt \ ../sfc_sice.f \ ### Ocean Surface ../sfc_nst.f \ + ../module_nst_model.f90 \ + ../module_nst_water_prop.f90 \ + ../module_nst_parameters.f90 \ ### Orographic Gravity Wave ../gwdps.f \ ### Convective Gravity Wave diff --git a/physics/docs/img/GFS_Operational_Physics.png b/physics/docs/img/GFS_Operational_Physics.png deleted file mode 100644 index 7ce7fdc4dc87e70a4afbcec3e1c8caebf5cb1402..0000000000000000000000000000000000000000 GIT binary patch literal 0 HcmV?d00001 literal 252976 zcmeFZXH=6*)G!(kM?D8A7MfI1QMv*mgsPw-peQ1tgMff^Nu-3X9zdjuAT5BXfJli* z36ZLlP!mKUNEHY~S|A1p5J>Km;5p*^erw&|cYSwQi&3=B>K9M9w)mX zI|u~g)W3Y;1_;DK0D=Bq{c8{K#G-TaZxARPq<`W3&49uA5zQEnp{x^YPOp@uz--aS zUH)mB$uH;i8iO(qxzV~#@vc7$I{I&mIZnDNA~jW8 zJKFgN=$00KjG&MuKcxXrU`hkjm^YaBP>2X={Yl}0C(6aiPm7b-KyUesyWlzTsnBdY zhB|8s>*T2A>Bx06yHNXYx)**n$dhWb6fKd};JfMoUdE^~g6>9b@*zg%4X$mxB%VEC z;4`NH#yqs={&yCOixak{8~1uB?F$;9@RpI_r>XaX^AIvMEH;E2lH0p~09=GMiT+E* zyT{FSZOD1s{E~R&0kU2|u47vR(^x?10`LA$M8oNN|366P)y*0a8 zeGH!`9{U#>I~W9tJs>j`tokF{(*@7Mv`0Nc_+R{t+jfC&6=wo75Wjk{RN=WlJNVzx zFA~{6jXeH(qo|Rua;&k-SH$)H

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zzx9KF$yn46er9cffN&PVkkGa3n?nbXm9-uDXD?6<;|y=_rsx{e9kKe15G&JQ0?veh z34tFT1T=GTvzgyaQgO5LX8!#N0h6(~Kfjj;Z&X(1LJwR*`HFBu8&^sGKO-u-u6Z>f zU_zkbLO|$1U0R@@>q;IQE)*K}%uL3jVSm5(c6KBf;ua>vK@*4?A|gki-`nAsy_pa& zAz(tlguuOrfXP_gdzk+qdK892l4dY|5R*11X+pq+fC&K;0x-Qo%pbvBfq=fKA4*&oF diff --git a/physics/docs/library.bib b/physics/docs/library.bib index 3e0be6b7b..7f7fcf3c0 100644 --- a/physics/docs/library.bib +++ b/physics/docs/library.bib @@ -1,13 +1,32 @@ %% This BibTeX bibliography file was created using BibDesk. %% http://bibdesk.sourceforge.net/ -%% Created for Man Zhang at 2018-01-31 17:02:44 -0700 +%% Created for Man Zhang at 2018-02-14 15:01:01 -0700 %% Saved with string encoding Unicode (UTF-8) +@book{pond_and_pickard_1983, + Author = {S. Pond and G.L. Pickard}, + Date-Added = {2018-02-14 21:57:02 +0000}, + Date-Modified = {2018-02-14 22:00:44 +0000}, + Edition = {2nd}, + Publisher = {Pergamon Press }, + Title = {Introductory dynamical oceanography}, + Year = {1983}} + +@article{zeng_et_al_1998, + Author = {X. Zeng and M. Zhao and R.E. Dickinson}, + Date-Added = {2018-02-13 23:09:56 +0000}, + Date-Modified = {2018-02-13 23:12:08 +0000}, + Journal = {J. Climate}, + Pages = {2628-2644}, + Title = {Intercomparison of bulk aerodynamic algorithm for the comutation of sea surface Fluxes using TOGA COARE and TAO data}, + Volume = {11}, + Year = {1998}} + @article{dorman_and_sellers_1989, Author = {J. L. Dorman and P. J. Sellers}, Date-Added = {2018-01-31 23:58:04 +0000}, diff --git a/physics/docs/txt/GFS_GWDC.txt b/physics/docs/txt/GFS_GWDC.txt index 08926e5cb..7982f167a 100644 --- a/physics/docs/txt/GFS_GWDC.txt +++ b/physics/docs/txt/GFS_GWDC.txt @@ -1,34 +1,6 @@ /** \page GFS_GWDC GFS Convective Gravity Wave Drag Scheme \section des_gwdc 1. Description - The GFS orographic gravity wave drag parameterization calculates the - effect of gravity waves produced by uneven distribution of diabatic - heat sources asscociated with convective systems on the - horizontal wind. - - At present, global models must be run with horizontal resolutions - that cannot typically resolve atmospheric phenomena shorter than - ~10-100 km or greater for weather prediction and ~100-1000 km or - greater for climate predicition. Many atmospheric processes have - shorter horizontal scales than these "subgrid-scale" processes - interact with and affect the larger-scale atmosphere in important - ways. - - Atmospheric gravity waves are one such unresolved processes. These - waves are generated by lower atmospheric sources. e.g., flow over - irregularities at the Earth's surface such as mountains and valleys, - uneven distribution of diabatic heat sources asscociated with - convective systems, and highly dynamic atmospheric processes such - as jet streams and fronts. The dissipation of these waves produces - synoptic-scale body forces on the atmospheric flow, known as - "gravity wave drag"(GWD), which affects both short-term evolution - of weather systems and long-term climate. However, the spatial - scales of these waves (in the range of ~5-500 km horizontally) are - too short to be fully captured in models, and so GWD must be - parameterized. In addition, the role of GWD in driving the global - middle atmosphere circulation and thus global mean wind/temperature - structures is well established. Thus, GWD parametrizations are now - critical components of virtually all large-scale atmospheric models. GFS physics includes parameterizations of gravity waves from two important sources: mountains and convection. This parameterization addresses the latter. @@ -49,19 +21,35 @@ the stable stratosphere can generate gravity waves that influence the large-scale flow. -\subsection provenance_gwdc Provenance - The parameterization of stationary convectively-forced GWD follows - the development of Chun and Baik (1998) \cite chun_and_baik_1998 , - which was tested in GCMs by Chun et al. (2001,2004) - \cite chun_et_al_2001 \cite chun_et_al_2004 was implemented in GFS - by Ake Johansson (2008) and the work of the GCWMB staff. Modest - positive effects from using the parameterization are seen in the - tropical upper troposphere and lower stratosphere. + Parameterizing subgrid-scale convection-induced gravity wave + momentum flux for use in large-scale models inherently requires + some information from subgrid-scale cumulus parameterization. + The methodology for parameterizing the zonal momentum flux induced + by thermal forcing can be summarized as follows. From the cloud-base + to cloud-top height, the effect of the momentum flux + induced by subgrid-scale diabatic forcing is not considered because + subgrid-scale cumulus convection in large-scale models is only + activated in a conditionally unstable atmosphere. Below the cloud + base, the momentum flux is also not considered because of the wave + momentum cancellation. At the cloud top, the momentum flux is + obtained by eq.(18) and (19) in Chun and Baik (1998) + \cite chun_and_baik_1998. Above the cloud top, there are two ways to + construct the momentum flux profile. One way is to specify a + vertical structure of the momentum flux normalized by the cloud-top + value, similar to what has been done for mountain drag + parameterization. The other way is to apply the wave saturation + hypothesis in order to find wave breaking levels in terms of the + Richardon number criterion using the nonlinearity factor of + thermally induced waves. \section intra_gwdc 2. Intraphysics Communication -\ref arg_table_gwdc_run +\sa \ref arg_table_gwdc_run + +\section gena_gwdc 3. General Algorithm +\sa \ref gen_gwdc -\section gen_gwdc 3. General Algorithm +\section det_gwdc 4. Detailed Algorithm +\sa \ref al_gwdc diff --git a/physics/docs/txt/GFS_GWDPS.txt b/physics/docs/txt/GFS_GWDPS.txt index 29f78a708..20b400aa1 100644 --- a/physics/docs/txt/GFS_GWDPS.txt +++ b/physics/docs/txt/GFS_GWDPS.txt @@ -92,10 +92,13 @@ \section intra_gwdps 2. Intraphysics Communication -\ref arg_table_gwdps_run +\sa \ref arg_table_gwdps_run \section gen_al_gwdps 3. General Algorithm +\sa \ref gen_gwdps +\section detailed_al_gwdps 4. Detailed Algorithm +\sa \ref det_gwdps */ diff --git a/physics/docs/txt/GFS_NSST.txt b/physics/docs/txt/GFS_NSST.txt index f8db1f130..7cdc4d336 100644 --- a/physics/docs/txt/GFS_NSST.txt +++ b/physics/docs/txt/GFS_NSST.txt @@ -10,22 +10,30 @@ This profile is a composed by subdividing the near-surface layer in three parts T(z) = Tr + T’w (z) + T’c (z), where -Ts = T(z=0) is the SST -T’c (z) is the temperature profile in the skin layer (0 < z <= zc) -T’w (z) is the temperature profile in the warm layer (0 < z <= zr) -Tr is the reference temperature -zc is the depth of the skin layer +\n Ts = T(z=0) is the SST +\n T’c (z) is the temperature profile in the skin layer (0 < z <= zc) +\n T’w (z) is the temperature profile in the warm layer (0 < z <= zr) +\n Tr is the reference temperature +\n zc is the depth of the skin layer -Prediction for the skin layer is made using the Thermal Skin-layer Model (TSM), while prediction for the thermocline is based on the Diurnal Thermocline Model (DTM), both with an origin on Fairall et al. (1996) \cite Fairall_all_1996. Atmospheric inputs include short- and long-wave radiation, surface pressure, surface layer winds, temperature and specific humidity, and rainfall. +Prediction for the skin layer is made using the Thermal Skin-layer Model (TSM), while prediction for the thermocline is based on the Diurnal Thermocline Model (DTM \ref nst_module), both with an origin on Fairall et al. (1996) \cite Fairall_all_1996. Atmospheric inputs include short- and long-wave radiation, surface pressure, surface layer winds, temperature and specific humidity, and rainfall. - \htmlonly - \endhtmlonly @image html NSST.png "Figure 1: NSST profile." +This scheme includes the following components: ++ \ref gfs_nst_main ++ \ref nst_water_prop ++ \ref nst_module ++ \ref nst_parameters + \section intra_nst 2. Intraphysics Communication -\ref arg_table_sfc_nst_run +\sa \ref arg_table_sfc_nst_run \section gen_nst 3. General Algorithm +\sa \ref NSST_general_algorithm + +\section det_nst 4. Detailed Algorithm +\sa \ref NSST_detailed_algorithm diff --git a/physics/docs/txt/GFS_SFCLYR.txt b/physics/docs/txt/GFS_SFCLYR.txt index aa4002c0d..20a20e174 100644 --- a/physics/docs/txt/GFS_SFCLYR.txt +++ b/physics/docs/txt/GFS_SFCLYR.txt @@ -1,23 +1,23 @@ /** -\page GFS_SFCLYR GFS Surface Roughness Length Calculation +\page GFS_SFCLYR GFS Surface Sublayer Scheme \section des_rough 1. Description - It is the surface roughness length formulation based on + It is the surface roughness length calculation based on the surface sublayer scheme from Zeng and Dickinson (1998) \cite zeng_and_dickinson_1998. - NOAH LSM are largely responsible for the quality + \ref NOAH are largely responsible for the quality of model forecasts produced for near-surface weather parameters, such - as 2-meter air temperature (\a T2m) and surface skin temperature - (\a LST). LST is derived from the surface energy budget, and is + as 2-meter air temperature (\f$T_{2m}\f$) and surface skin temperature + (\f$LST\f$). \f$LST\f$ is derived from the surface energy budget, and is particularly important to remote sensing and data assimilation. How precise these two parameters can be simulated by the model strongly - dependes on how accurate the surface heat fluxes are parameterized, - particularly the surface sensible heat flux (\a SH). The surface - thermal roughness length is a key parameter to determine \a SH. + depends on how accurate the surface heat fluxes are parameterized, + particularly the surface sensible heat flux (\f$SH\f$). The surface + thermal roughness length is a key parameter to determine \f$SH\f$. Previous GFS version do not distinguish between the roughness length for heat and momentum. The aerodynamic roughness \f$Z_{0m}\f$ is used for wind, while the thermal roughness \f$Z_{0t}\f$ is used for heat and - water vapor. In general,\f$Z_{0m}\f$ is different from \f$Z_{0t}\f$, + water vapor. In general, \f$Z_{0m}\f$ is different from \f$Z_{0t}\f$, because the transfer of momentum is affected by pressure fluctuations in the turbulent waves behind the roughness elements, while for heat and water vapor transfer no such dynamical mechanism exists. Zeng and @@ -27,35 +27,16 @@ in the desert summer afternoon. In May 2011, the new vegetation-dependent formulations of - momentum and thermal roughness formulation (Zheng et al. 2009 + thermal roughness formulation (Zheng et al. 2009 \cite zheng_et_al_2009; Zheng et al. 2012 \cite zheng_et_al_2012 ) - was implemented to deal with the cold LST bias + was implemented to deal with the cold \f$LST\f$ bias over the arid western continental United States - (CONUS) during daytime. This LST bias contributes to large errors in + (CONUS) during daytime. This \f$LST\f$ bias contributes to large errors in simulated satellite brightness temperatures over land by the Community Radiative Transfer Model (CRTM) and hence the rejection of satellite data in the NCEP Gridpoint Statistical Interpolation (GSI) system, especially for surface-sensitive satellite channels. - Zheng et al.(2009) \cite zheng_et_al_2009 proposed a new formulation on - \f$ln(Z_{0m}^,/Z_{0t})\f$ as follows: -\f[ - ln(Z_{0m}^,/Z_{0t})=(1-GVF)^2C_{zil}k(u*Z_{0g}/\nu)^{0.5} -\f] - where \f$Z_{0m}^,\f$ is the effective momentum roughness length - computed in the following equation for each grid, \f$Z_{0t}\f$ - is the roughness lenghth for heat, \f$C_{zil}\f$ is a coefficient - (taken as 0.8), k is the Von Karman constant (0.4), - \f$\nu=1.5\times10^{-5}m^{2}s^{-1}\f$ is the molecular viscosity, - \f$u*\f$ is the friction velocity, and \f$Z_{0g}\f$ is the bare - soil roughness length for momentum (taken as 0.01). - \n In order to consider the convergence of \f$Z_{0m}\f$ between - fully vegetated and bare soil, the effective \f$Z_{0m}^,\f$ is - computed: -\f[ - \ln(Z_{0m}^,)=(1-GVF)^{2}\ln(Z_{0g})+\left[1-(1-GVF)^{2}\right]\ln(Z_{0m}) -\f] - \image html roughness_length_fig1.png "Figure 1: Comparison of LST simulated in GFS and verification with the observations. (a) Difference between GFS and GOES in the control run at 18:00 UTC; (b) Difference between GFS and GOES with the new formulation run at 18:00 UTC, averaged from 1 to 3 July 2007" width=10cm Figure 1 show the 3 day average land surface skin temperature predicted @@ -64,23 +45,24 @@ the control run (Figure 1a), a substantial cold bias can be found over the west half of CONUS (i.e., arid or semiarid regions). The new roughness length formulations significantly reduce the cold bias in the western - CONUS, while the LST in the eastern CONUS, where the bias is small in + CONUS, while the \f$LST\f$ in the eastern CONUS, where the bias is small in the control run, is not much affected. \image html roughness_length_fig2.png "Fiure 2: Average diurnal cycle on 1-3 July 2007 for verification of LST with GOES (black) and SURFRAD (blue) at Desert Rock, Nevada; red and green lines are for the control and sensitivity runs, respectively" width=10cm The Desert Rock station (\f$36.63^oN\f$, \f$116.02^oW\f$), located in the Nevada desert,is one of the observation stations within the SURFRAD network. - The GOES-derived LST is very similar to the SURFRAD obervations (Figure 2). - However, the old GFS run produces very low LST, compared to the observations, + The GOES-derived \f$LST\f$ is very similar to the SURFRAD obervations (Figure 2). + However, the old GFS run produces very low \f$LST\f$, compared to the observations, especially during daytime. During midday, the cold bias can reach up to - \f$-15^oC\f$. The new formulation run produces a reasonable LST diurnal cycle. - The daytime LST increases substantially and is very close to the observations. + \f$-15^oC\f$. The new formulation run produces a reasonable \f$LST\f$ diurnal cycle. + The daytime \f$LST\f$ increases substantially and is very close to the observations. \section intra_rough 2. Intraphysics Communication -\ref arg_table_sfc_ex_coef_run +\sa \ref arg_table_sfc_ex_coef_run \section gen_rough 3. General Algorithm +\sa \ref general_diff diff --git a/physics/docs/txt/GFS_SFCSICE.txt b/physics/docs/txt/GFS_SFCSICE.txt index ad71d7cb1..19eebddc9 100644 --- a/physics/docs/txt/GFS_SFCSICE.txt +++ b/physics/docs/txt/GFS_SFCSICE.txt @@ -1,5 +1,5 @@ /** -\page GFS_SFCSICE GFS Three-Layer Thermodynamics Sea Ice Scheme +\page GFS_SFCSICE GFS Sea Ice Scheme \section des_sice 1. Description This is three-layer thermodynomics sea-ice model based on Winton (2000) \cite winton_2000. @@ -46,12 +46,12 @@ The model consists of a zero-heat-capacity snow layer overlying two equally thick sea ice layers (Fig.1). The upper ice layer has a variable heat capacity to represent brine pockets. -\image html schematic_sice.png "Fig.2 NCEP Sea Ice Model System Diagram" width=10cm - \section intra_sice 2. Intraphysics Communication -\ref arg_table_sfc_sice_run +\image html schematic_sice.png "Fig.2 NCEP Sea Ice Model System Diagram" width=10cm +\sa \ref arg_table_sfc_sice_run \section gen_sice 3. General Algorithm +\sa \ref general_sice_run diff --git a/physics/docs/txt/GFS_ZHAOC.txt b/physics/docs/txt/GFS_ZHAOC.txt index 1682d2ced..8fdd58bd8 100644 --- a/physics/docs/txt/GFS_ZHAOC.txt +++ b/physics/docs/txt/GFS_ZHAOC.txt @@ -1,7 +1,7 @@ /** \page GFS_ZHAOC GFS Zhao-Carr Microphysics Scheme \section des_zhao 1. Description - This is the GFS scheme for large-scale condensation and precipitation which is based on + This is the GFS scheme for grid-scale condensation and precipitation which is based on Zhao and Carr (1997) \cite zhao_and_carr_1997 and Sundqvist et al.(1989) \cite sundqvist_et_al_1989 . The main feature of this parameterization is the inclusion of cloud water and cloud ice in both the convective and grid-scale precipitation paramterizations, and use only one predictive variable, the diff --git a/physics/gscond.f b/physics/gscond.f index 556245bf9..2502fb653 100644 --- a/physics/gscond.f +++ b/physics/gscond.f @@ -49,11 +49,11 @@ end subroutine gscond_init !! !> \section general_gscond General Algorithm !! -# Calculate ice-water identification number \f$IW\f$ in order to make a distinction betwee -!! cloud water and cloud ice (table2 in Zhao and Carr (1997)). +!! cloud water and cloud ice (table2 of Zhao and Carr (1997) \cite zhao_and_carr_1997). !! -# Calculate the changes in \f$t\f$, \f$q\f$ and \f$p\f$ due to all the processes except microphysics. -!! -# Calculate cloud evaporation process (\f$E_c\f$) -!! \todo general_gscond -!!\n Cloud evaporation is allowed to take place only where +!! -# Calculate cloud evaporation rate (\f$E_c\f$, eq. 19 of Zhao and Carr (1997) \cite zhao_and_carr_1997) +!! -# Calculate cloud condensation rate (\f$C_g\f$, eq.8 of Zhao and Carr (1997) \cite zhao_and_carr_1997) +!! -# update t,q,cwm due to cloud evaporation and condensation process !> \section Zhao-Carr_cond_detailed Detailed Algorithm !> @{ subroutine gscond_run (im,ix,km,dt,dtf,prsl,ps,q,clw1,clw2 & @@ -315,7 +315,7 @@ subroutine gscond_run (im,ix,km,dt,dtf,prsl,ps,q,clw1,clw2 & !! E_{c}=\frac{cwm}{dt} !! \f] !! - If cloud fraction \f$b>1.0\times10^{-3}\f$, condense water vapor -!! in to cloud condensate (\f$C_{g}\f$). +!! into cloud condensate (\f$C_{g}\f$). !!\n Using \f$q=fq_{s}\f$, \f$q_{s}=\epsilon e_{s}/p\f$, and the !! Clausius-Clapeyron equation \f$de_{s}/dT=\epsilon Le_{s}/RT^{2}\f$, !! where \f$q_{s}\f$ is the saturation specific humidity,\f$e_{s}\f$ diff --git a/physics/gwdc.f b/physics/gwdc.f index d888e5836..4161179c4 100644 --- a/physics/gwdc.f +++ b/physics/gwdc.f @@ -2,67 +2,6 @@ !! stationary convection forced gravity wave drag based on Chun and !! Baik(1998) \cite chun_and_baik_1998 -!> \defgroup GFS_cgwd GFS Convective Gravity Wave Drag -!! @{ -!! The GFS orographic gravity wave drag parameterization calculates the -!! effect of gravity waves produced by uneven distribution of diabatic -!! heat sources asscociated with convective systems on the -!! horizontal wind. -!! -!! At present, global models must be run with horizontal resolutions -!! that cannot typically resolve atmospheric phenomena shorter than -!! ~10-100 km or greater for weather prediction and ~100-1000 km or -!! greater for climate predicition. Many atmospheric processes have -!! shorter horizontal scales than these "subgrid-scale" processes -!! interact with and affect the larger-scale atmosphere in important -!! ways. -!! -!! Atmospheric gravity waves are one such unresolved processes. These -!! waves are generated by lower atmospheric sources. e.g., flow over -!! irregularities at the Earth's surface such as mountains and valleys, -!! uneven distribution of diabatic heat sources asscociated with -!! convective systems, and highly dynamic atmospheric processes such -!! as jet streams and fronts. The dissipation of these waves produces -!! synoptic-scale body forces on the atmospheric flow, known as -!! "gravity wave drag"(GWD), which affects both short-term evolution -!! of weather systems and long-term climate. However, the spatial -!! scales of these waves (in the range of ~5-500 km horizontally) are -!! too short to be fully captured in models, and so GWD must be -!! parameterized. In addition, the role of GWD in driving the global -!! middle atmosphere circulation and thus global mean wind/temperature -!! structures is well established. Thus, GWD parametrizations are now -!! critical components of virtually all large-scale atmospheric models. -!! GFS physics includes parameterizations of gravity waves from two -!! important sources: mountains and convection. This parameterization -!! addresses the latter. -!! -!! In a review paper on gravity waves in the middle atmosphere, Fritts -!! (1984) \cite fritts_1984 showed that a large portion of observed -!! gravity wave momentum flux has higher frequencies than those of -!! stationary mountain waves. This phenomenon was explained by cumulus -!! convection, which is an additional source of tropospheric gravity -!! waves, and is particularly important in summertime. When the surface -!! wind and stability are weak, the magnitude of the surface drag and -!! the resultant influence of orographically-induced gravity wave drag -!! on the large-scale flow are relatively small compared with those in -!! wintertime (Palmer et al. 1986 \cite palmer_et_al_1986). In this -!! situation, the relative importance of cumulus convection as a source -!! of gravity waves is larger. In addition, in the tropical regions -!! where persistent convection exists, deep cumulus clouds impinging on -!! the stable stratosphere can generate gravity waves that influence -!! the large-scale flow. -!! -!> \section provenance_gwdc Provenance -!! - The parameterization of stationary convectively-forced GWD follows -!! the development of Chun and Baik (1998) \cite chun_and_baik_1998 , -!! which was tested in GCMs by Chun et al. (2001,2004) -!! \cite chun_et_al_2001 \cite chun_et_al_2004 was implemented in GFS -!! by Ake Johansson (2008) and the work of the GCWMB staff. Modest -!! positive effects from using the parameterization are seen in the -!! tropical upper troposphere and lower stratosphere. -!! -!> \section intraphysics Intraphysics Communication - module gwdc_pre contains @@ -165,33 +104,14 @@ module gwdc subroutine gwdc_init() end subroutine gwdc_init +!> \defgroup GFS_cgwd GFS Convective Gravity Wave Drag !> \defgroup GFS_gwdc_run GFS gwdc Main +!! \ingroup GFS_cgwd !! \brief This subroutine is the parameterization of convective gravity wave !! drag based on the theory given by Chun and Baik (1998) !! \cite chun_and_baik_1998 modified for implementation into the !! GFS/CFS by Ake Johansson(Aug 2005). !! -!> Parameterizing subgrid-scale convection-induced gravity wave -!! momentum flux for use in large-scale models inherently requires -!! some information from subgrid-scale cumulus parameterization. -!! The methodology for parameterizing the zonal momentum flux induced -!! by thermal forcing can be summarized as follows. From the cloud-base -!! to cloud-top height, the effect of the momentum flux -!! induced by subgrid-scale diabatic forcing is not considered because -!! subgrid-scale cumulus convection in large-scale models is only -!! activated in a conditionally unstable atmosphere. Below the cloud -!! base, the momentum flux is also not considered because of the wave -!! momentum cancellation. At the cloud top, the momentum flux is -!! obtained by eq.(18) and (19) in Chun and Baik (1998) -!! \cite chun_and_baik_1998. Above the cloud top, there are two ways to -!! construct the momentum flux profile. One way is to specify a -!! vertical structure of the momentum flux normalized by the cloud-top -!! value, similar to what has been done for mountain drag -!! parameterization. The other way is to apply the wave saturation -!! hypothesis in order to find wave breaking levels in terms of the -!! Richardon number criterion using the nonlinearity factor of -!! thermally induced waves. -!! !! \section arg_table_gwdc_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|--------------------------------------------------------|--------------------------------------------------------------------|------------|------|---------|-----------|--------|----------| @@ -227,7 +147,9 @@ end subroutine gwdc_init !! | tauctx | instantaneous_x_stress_due_to_gravity_wave_drag | zonal stress at cloud top due to convective gravity wave drag | Pa | 1 | real | kind_phys | out | F | !! | taucty | instantaneous_y_stress_due_to_gravity_wave_drag | meridional stress at cloud top due to convective gravity wave drag | Pa | 1 | real | kind_phys | out | F | !! -!> \section al_gwdc General Algorithm +!> \section gen_gwdc General Algorithm +!! +!> \section al_gwdc Detailed Algorithm !> @{ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & & pmid1,pint1,dpmid1,qmax,ktop,kbot,kcnv,cldf, & @@ -1617,4 +1539,3 @@ end subroutine gwdc_post_finalize end module gwdc_post -!> @} diff --git a/physics/gwdps.f b/physics/gwdps.f index 557ed6b40..2dacce802 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -2,115 +2,16 @@ !! This file is the parameterization of orographic gravity wave !! drag and mountain blocking. -!> \defgroup GFS_ogwd GFS Orographic Gravity Wave Drag -!! @{ -!! The GFS orographic gravity wave drag parameterization calculates the -!! effect of gravity waves produced by flow over irregularities at the -!! Earth's surface such as mountains and valleys and highly dynamic -!! atmospheric processes such as jet streams and fronts on the -!! horizontal wind. -!! -!! At present, global models must be run with horizontal resolutions -!! that cannot typically resolve atmospheric phenomena shorter than -!! ~10-100 km or greater for weather prediction and ~100-1000 km or -!! greater for climate predicition. Many atmospheric processes have -!! shorter horizontal scales than these "subgrid-scale" processes -!! interact with and affect the larger-scale atmosphere in important -!! ways. -!! -!! Atmospheric gravity waves are one such unresolved processes. These -!! waves are generated by lower atmospheric sources. e.g., flow over -!! irregularities at the Earth's surface such as mountains and valleys, -!! uneven distribution of diabatic heat sources asscociated with -!! convective systems, and highly dynamic atmospheric processes such -!! as jet streams and fronts. The dissipation of these waves produces -!! synoptic-scale body forces on the atmospheric flow, known as -!! "gravity wave drag"(GWD), which affects both short-term evolution -!! of weather systems and long-term climate. However, the spatial -!! scales of these waves (in the range of ~5-500 km horizontally) are -!! too short to be fully captured in models, and so GWD must be -!! parameterized. In addition, the role of GWD in driving the global -!! middle atmosphere circulation and thus global mean wind/temperature -!! structures is well established. Thus, GWD parametrizations are now -!! critical components of virtually all large-scale atmospheric models. -!! GFS physics includes parameterizations of gravity waves from two -!! important sources: mountains and convection. This parameterization -!! address the former. -!! -!! Atmospheric flow is significantly influenced by orography creating -!! lift and frictional forces. The representation of orography and its -!! influence in numerical weather prediction models are necessarily -!! divided into the resolvable scales of motion and treated by -!! primitive equations, the remaining sub-grid scales to be treated by -!! parameterization. In terms of large scale NWP models, mountain -!! blocking of wind flow around sub-grid scale orograph is a process -!! that retards motion at various model vertical levels near or in the -!! boundary layer. Flow around the mountain encounters larger -!! frictional forces by being in contact with the mountain surfaces -!! for longer time as well as the interaction of the atmospheric -!! environment with vortex shedding which occurs in numerous -!! observations. Lott and Miller (1997) \cite lott_and_miller_1997, -!! incorporated the dividing streamline and mountain blocking in -!! conjunction with sub-grid scale vertically propagating gravity wave -!! parameterization in the context of NWP. The dividing streamline is -!! seen as a source of gravity waves to the atmosphere above and -!! nonlinear subgrid low-level mountain drag effect below. -!! -!> \section provenance_gwdps Provenance -!! - Gravity-wave drag is simulated as described by Alpert et al. -!! (1988) \cite alpert_et_al_1988. The parameterization includes -!! determination of the momentum flux due to gravity waves at the -!! surface, as well as upper levels. The surface stress is a nonlinear -!! function of the surface wind speed and the local Froude number, -!! following Pierrehumbert (1987) \cite pierrehumbert_1987. Vertical -!! variations in the momentum flux occur when the local Richardson -!! number is less than 0.25 (the stress vanishes), or when wave -!! breaking occurs (local Froude number becomes critical); in the -!! latter case, the momentum flux is reduced according to the -!! Lindzen(1981) \cite lindzen_1981 wave saturation hypothesis. -!! Modifications are made to avoid instability when the critical layer -!! is near the surface, since the time scale for gravity-wave drag is -!! shorter than the model time step. -!! -!! - The treatment of the GWD in the lower troposphere is enhanced -!! according to Kim and Arakawa (1995) \cite kim_and_arakawa_1995 . -!! Orographic Std Dev (HPRIME), Convexity(OC), Asymmetry (OA4) and Lx -!! (CLX4) are input topographic statistics needed (see Appendix in Kim -!! and Arakawa (1995) \cite kim_and_arakawa_1995) . -!! -!! - Mountain blocking influences are incorporated following the Lott -!! and Miller (1997) \cite lott_and_miller_1997 parameterization with -!! minor changes, including their dividing streamline concept. The -!! model subgrid scale orography is represented by four parameters, -!! after Baines and Palmer (1990) \cite baines_and_palmer_1990, the -!! standard deviation (HPRIME), the anisotropy (GAMMA), the slope -!! (SIGMA) and the geographical orientation of the orography (THETA). -!! These are calculated off-line as a function of model resolution in -!! the fortran code ml01rg2.f, with script mlb2.sh (see Appendix: -!! Specification of subgrid-scale orography in Lott and Miller (1997) -!! \cite lott_and_miller_1997). -!! -!! - The orographic GWD parameterizations automatically scales -!! with model resolution. For example, the T574L64 version of GFS uses -!! four times stronger mountain blocking and one half the strength of -!! gravity wave drag than the T383L64 version. -!! -!> \section intraphysics Intraphysics Communication module gwdps_pre contains -! \ingroup GFS_ogwd -! \brief Brief description of the subroutine -! ! \section arg_table_gwdps_pre_init Argument Table ! subroutine gwdps_pre_init() end subroutine gwdps_pre_init -! \ingroup GFS_ogwd -! \brief Brief description of the subroutine ! ! \section arg_table_gwdps_pre_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -216,14 +117,12 @@ module gwdps contains -! \ingroup GFS_ogwd -! \brief Brief description of the subroutine -! ! \section arg_table_gwdps_init Argument Table ! subroutine gwdps_init() end subroutine gwdps_init +!> \defgroup GFS_ogwd GFS Orographic Gravity Wave Drag !> \defgroup gfs_gwdps GFS gwdps Main !!\ingroup GFS_ogwd !! \brief This subroutine includes orographic gravity wave drag and mountain @@ -279,6 +178,8 @@ end subroutine gwdps_init !! | ipr | horizontal_index_of_printed_column | horizontal index of column used in debugging printouts | index | 0 | integer | default | in | F | !! !> \section gen_gwdps General Algorithm +!! -# Calculate subgrid mountain blocking +!! -# Calculate orographic wave drag !> \section det_gwdps Detailed Algorithm !> @{ subroutine gwdps_run( & @@ -538,7 +439,7 @@ subroutine gwdps_run( & ! & print *,' in gwdps_lm.f npt,IM,IX,IY,km,me=',npt,IM,IX,IY,km,me ! ! -!> --- Subgrid Mountain Blocking Section +!>-# Subgrid Mountain Blocking Section ! !.............................. !.............................. @@ -817,7 +718,7 @@ subroutine gwdps_run( & !............................. !............................. ! -!> --- Orographic Gravity Wave Drag Section +!>-# Orographic Gravity Wave Drag Section KMPBL = km / 2 ! maximum pbl height : # of vertical levels / 2 ! ! Scale cleff between IM=384*2 and 192*2 for T126/T170 and T62 @@ -1341,8 +1242,6 @@ subroutine gwdps_run( & end subroutine gwdps_run !> @} -! \ingroup GFS_ogwd -! \brief Brief description of the subroutine ! ! \section arg_table_gwdps_finalize Argument Table ! @@ -1357,15 +1256,11 @@ module gwdps_post contains -! \ingroup GFS_ogwd -! \brief Brief description of the subroutine -! ! \section arg_table_gwdps_post_init Argument Table ! subroutine gwdps_post_init() end subroutine gwdps_post_init -! \ingroup GFS_ogwd ! \brief Brief description of the subroutine ! \section arg_table_gwdps_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -1412,14 +1307,9 @@ subroutine gwdps_post_run( & end subroutine gwdps_post_run -! \ingroup GFS_ogwd -! \brief Brief description of the subroutine -! ! \section arg_table_gwdps_post_finalize Argument Table ! subroutine gwdps_post_finalize() end subroutine gwdps_post_finalize end module gwdps_post - -!> @} diff --git a/physics/module_nst_model.f90 b/physics/module_nst_model.f90 index f2b05c110..4f83077fd 100644 --- a/physics/module_nst_model.f90 +++ b/physics/module_nst_model.f90 @@ -1,3 +1,8 @@ +!>\file module_nst_model.f90 +!>\defgroup nst_module Diurnal Thermocline Model +!! @{ +!>\ingroup GFS_NSST +!!\brief This is the module of diurnal thermocline layer model (DTM). module nst_module ! @@ -921,4 +926,4 @@ end subroutine dtl_reset end module nst_module - +!! @ } diff --git a/physics/module_nst_parameters.f90 b/physics/module_nst_parameters.f90 index 1186177e4..4845c383f 100644 --- a/physics/module_nst_parameters.f90 +++ b/physics/module_nst_parameters.f90 @@ -1,3 +1,7 @@ +!>\file module_nst_parameters.f90 +!>\defgroup nst_parameters NST Parameters Module +!! \ingroup GFS_NSST +!! @{ module module_nst_parameters use machine, only : kind_phys & ,kind_rad ! for astronomy (date) calculations @@ -141,3 +145,4 @@ module module_nst_parameters !!$ !!$ end module module_nst_parameters +!! @} diff --git a/physics/module_nst_water_prop.f90 b/physics/module_nst_water_prop.f90 index f31d97241..2f4d5df6d 100644 --- a/physics/module_nst_water_prop.f90 +++ b/physics/module_nst_water_prop.f90 @@ -1,3 +1,8 @@ +!>\file module_nst_water_prop.f90 +!>\defgroup nst_water_prop NST Water Prop Module +!! @{ +!>\ingroup GFS_NSST +!!\brief module module_nst_water_prop use machine, only : kind_phys use module_nst_parameters, only : t0k @@ -34,6 +39,8 @@ module module_nst_water_prop end interface contains ! ------------------------------------------------------ +!> This subroutine computes thermal expansion coefficient (alpha) +!! and saline contraction coefficient (beta). subroutine rhocoef(t, s, rhoref, alpha, beta) ! ------------------------------------------------------ @@ -76,6 +83,7 @@ subroutine rhocoef(t, s, rhoref, alpha, beta) end subroutine rhocoef ! ---------------------------------------- +!> This subroutine computes sea water density. subroutine density(t, s, rho) ! ---------------------------------------- implicit none @@ -112,6 +120,8 @@ end subroutine density ! !====================== ! +!> This subroutine computes the fraction of the solar radiation absorbed +!! by the depth z following Paulson and Simpson (1981) \cite paulson_and_simpson_1981 . elemental subroutine sw_ps_9b(z,fxp) ! ! fraction of the solar radiation absorbed by the ocean at the depth z @@ -447,6 +457,7 @@ function grv(lat) !print *,'grav=',grv,lat end function grv +!>This subroutine computes solar time from the julian date. subroutine solar_time_from_julian(jday,xlon,soltim) ! ! calculate solar time from the julian date @@ -470,6 +481,8 @@ end subroutine solar_time_from_julian ! !*********************************************************************** ! +!> This subroutine computes julian day and fraction from year, +!! month, day and time UTC. subroutine compjd(jyr,jmnth,jday,jhr,jmn,jd,fjd) !fpp$ noconcur r !$$$ subprogram documentation block @@ -517,6 +530,7 @@ subroutine compjd(jyr,jmnth,jday,jhr,jmn,jd,fjd) endif end subroutine compjd +!>This subroutine computes dtm (the mean of \f$dT(z)\f$). subroutine get_dtzm_point(xt,xz,dt_cool,zc,z1,z2,dtm) ! ===================================================================== ! ! ! @@ -701,3 +715,4 @@ subroutine get_dtzm_2d(xt,xz,dt_cool,zc,slmsk,z1,z2,nx,ny,dtm) end subroutine get_dtzm_2d end module module_nst_water_prop +!! @} diff --git a/physics/precpd.f b/physics/precpd.f index c2880e4db..0c92bd30d 100644 --- a/physics/precpd.f +++ b/physics/precpd.f @@ -1,6 +1,6 @@ !> \file precpd.f !! This file contains the subroutine that calculates precipitation -!! processes from suspended cloud water/ice +!! processes from suspended cloud water/ice. module GFS_zhaocarr_precpd contains @@ -43,7 +43,12 @@ end subroutine precpd_init !! | jpr | horizontal_index_of_printed_column | horizontal index of printed column | index | 0 | integer | | in | F | !! !> \section general_precpd General Algorithm -!! \todo general precpd +!! -# Calculate precipitation production by auto conversion and accretion (\f$P_{saut}\f$, \f$P_{saci}\f$, \f$P_{raut}\f$). +!! - The accretion of cloud water by rain, \f$P_{racw}\f$, is not included in the current operational scheme. +!! -# Calculate evaporation of precipitation (\f$E_{rr}\f$ and \f$E_{rs}\f$). +!! -# Calculate melting of snow (\f$P_{sm1}\f$ and \f$P_{sm2}\f$, \f$P_{sacw}\f$). +!! -# Update t and q due to precipitation (snow or rain) production. +!! -# Calculate precipitation at surface (\f$rn\f$) and fraction of frozen precipitation (\f$sr\f$). !! \section Zhao-Carr_precip_detailed Detailed Algorithm !! @{ subroutine precpd_run (im,ix,km,dt,del,prsl,q,cwm,t,rn,sr & @@ -334,7 +339,7 @@ subroutine precpd_run (im,ix,km,dt,del,prsl,q,cwm,t,rn,sr & ! if (tmt0(n).le.-40.) qint = qi ! !-------------------ice-water id number iw------------------------------ -!> -# Compute ice-water identification number IW (see algorithm in +!> -# Calculate ice-water identification number IW (see algorithm in !! \ref condense). if(tmt0(n) < -15.) then fi = qk - u00k(i,k)*qi @@ -465,15 +470,15 @@ subroutine precpd_run (im,ix,km,dt,del,prsl,q,cwm,t,rn,sr & praut = min(praut, cwmk) ww(n) = ww(n) - praut ! -!> - Calculate the accretion of cloud water by rain \f$P_{racw}\f$, -!! can be expressed using the cloud mixing ratio \f$cwm\f$ and rainfall -!! rate \f$P_{r}\f$: -!!\f[ -!! P_{saci}=C_{s}cwmP_{r} -!!\f] -!! where \f$C_{r}=5.0\times10^{-4}m^{2}kg^{-1}s{-1}\f$ is the -!! collection coeffiecient. Note that this process is not included in -!! current operational physcics. +! - Calculate the accretion of cloud water by rain \f$P_{racw}\f$, +! can be expressed using the cloud mixing ratio \f$cwm\f$ and rainfall +! rate \f$P_{r}\f$: +!\f[ +! P_{racw}=C_{r}cwmP_{r} +!\f] +! where \f$C_{r}=5.0\times10^{-4}m^{2}kg^{-1}s^{-1}\f$ is the +! collection coeffiecient. Note that this process is not included in +! current operational physcics. ! below is for zhao's precip formulation (water) ! ! amaxcm = max(cons_0, cwmk - wmink(n)) @@ -663,7 +668,7 @@ subroutine precpd_run (im,ix,km,dt,del,prsl,q,cwm,t,rn,sr & !-----------------------end of precipitation processes----------------- !********************************************************************** ! -!> -# Compute precipitation at surface (\f$rn\f$)and determine +!> -# Calculate precipitation at surface (\f$rn\f$)and determine !! fraction of frozen precipitation (\f$sr\f$). !!\f[ !! rn= (P_{r}(\eta_{sfc})+P_{s}(\eta_{sfc}))/10^3 diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index 90e358d83..6aa708f0d 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -1,86 +1,7 @@ !> \file sfc_diff.f !! This file contains the surface roughness length formulation based on !! the surface sublayer scheme from Zeng and Dickinson (1998) -!! \cite zeng_and_dickinson_1998. It is -!! the first subroutine called in surface layer loop. - -!> \defgroup Sfc_ex_cal GFS Surface Roughness Length Calculation -!! \brief It is the surface roughness length formulation based on -!! the surface sublayer scheme from Zeng and Dickinson (1998) -!! \cite zeng_and_dickinson_1998. -!! -!! NOAH LSM are largely responsible for the quality -!! of model forecasts produced for near-surface weather parameters, such -!! as 2-meter air temperature (\a T2m) and surface skin temperature -!! (\a LST). LST is derived from the surface energy budget, and is -!! particularly important to remote sensing and data assimilation. How -!! precise these two parameters can be simulated by the model strongly -!! dependes on how accurate the surface heat fluxes are parameterized, -!! particularly the surface sensible heat flux (\a SH). The surface -!! thermal roughness length is a key parameter to determine \a SH. -!! Previous GFS version do not distinguish between the roughness length -!! for heat and momentum. The aerodynamic roughness \f$Z_{0m}\f$ is used -!! for wind, while the thermal roughness \f$Z_{0t}\f$ is used for heat and -!! water vapor. In general,\f$Z_{0m}\f$ is different from \f$Z_{0t}\f$, -!! because the transfer of momentum is affected by pressure fluctuations -!! in the turbulent waves behind the roughness elements, while for heat -!! and water vapor transfer no such dynamical mechanism exists. Zeng and -!! Dickinson (1998) \cite zeng_and_dickinson_1998 found that the surface -!! skin temperature can be at least 10 K higher when considering the surface -!! sublayer (or the variable ratio of the \f$Z_{0m}/Z_{0t}\f$ than without -!! in the desert summer afternoon. -!! -!! In May 2011, the new vegetation-dependent formulations of -!! momentum and thermal roughness formulation (Zheng et al. 2009 -!! \cite zheng_et_al_2009; Zheng et al. 2012 \cite zheng_et_al_2012 ) -!! was implemented to deal with the cold LST bias -!! over the arid western continental United States -!! (CONUS) during daytime. This LST bias contributes to large errors in -!! simulated satellite brightness temperatures over land by the Community -!! Radiative Transfer Model (CRTM) and hence the rejection of satellite -!! data in the NCEP Gridpoint Statistical Interpolation (GSI) system, -!! especially for surface-sensitive satellite channels. -!! -!! Zheng et al.(2009) \cite zheng_et_al_2009 proposed a new formulation on -!! \f$ln(Z_{0m}^,/Z_{0t})\f$ as follows: -!!\f[ -!! ln(Z_{0m}^,/Z_{0t})=(1-GVF)^2C_{zil}k(u*Z_{0g}/\nu)^{0.5} -!!\f] -!! where \f$Z_{0m}^,\f$ is the effective momentum roughness length -!! computed in the following equation for each grid, \f$Z_{0t}\f$ -!! is the roughness lenghth for heat, \f$C_{zil}\f$ is a coefficient -!! (taken as 0.8), k is the Von Karman constant (0.4), -!! \f$\nu=1.5\times10^{-5}m^{2}s^{-1}\f$ is the molecular viscosity, -!! \f$u*\f$ is the friction velocity, and \f$Z_{0g}\f$ is the bare -!! soil roughness length for momentum (taken as 0.01). -!! \n In order to consider the convergence of \f$Z_{0m}\f$ between -!! fully vegetated and bare soil, the effective \f$Z_{0m}^,\f$ is -!! computed: -!!\f[ -!! \ln(Z_{0m}^,)=(1-GVF)^{2}\ln(Z_{0g})+\left[1-(1-GVF)^{2}\right]\ln(Z_{0m}) -!!\f] -!! -!!\image html roughness_length_fig1.png "Figure 1: Comparison of LST simulated in GFS and verification with the observations. (a) Difference between GFS and GOES in the control run at 18:00 UTC; (b) Difference between GFS and GOES with the new formulation run at 18:00 UTC, averaged from 1 to 3 July 2007" width=10cm -!! -!! Figure 1 show the 3 day average land surface skin temperature predicted -!! by the GFS and comparison with the GOES-derived satellite measurements. -!! At 18:00 UTC (midday in local time over the central United States) in -!! the control run (Figure 1a), a substantial cold bias can be found over -!! the west half of CONUS (i.e., arid or semiarid regions). The new roughness -!! length formulations significantly reduce the cold bias in the western -!! CONUS, while the LST in the eastern CONUS, where the bias is small in -!! the control run, is not much affected. -!! -!!\image html roughness_length_fig2.png "Fiure 2: Average diurnal cycle on 1-3 July 2007 for verification of LST with GOES (black) and SURFRAD (blue) at Desert Rock, Nevada; red and green lines are for the control and sensitivity runs, respectively" width=10cm -!! -!! The Desert Rock station (\f$36.63^oN\f$, \f$116.02^oW\f$), located in the Nevada -!! desert,is one of the observation stations within the SURFRAD network. -!! The GOES-derived LST is very similar to the SURFRAD obervations (Figure 2). -!! However, the old GFS run produces very low LST, compared to the observations, -!! especially during daytime. During midday, the cold bias can reach up to -!! \f$-15^oC\f$. The new formulation run produces a reasonable LST diurnal cycle. -!! The daytime LST increases substantially and is very close to the observations. -!! \section intraphysics Intraphysics Communication +!! \cite zeng_and_dickinson_1998. It is the first subroutine called in surface layer loop. module surface_exchange_coefficients contains @@ -91,8 +12,8 @@ end subroutine sfc_ex_coef_init subroutine sfc_ex_coef_finalize end subroutine sfc_ex_coef_finalize -! subroutine sfc_diff(im,ps,u1,v1,t1,q1,z1, - +!> \defgroup Sfc_ex_cal GFS Surface Sublayer Scheme +!! !> \defgroup GFS_diff_main GFS sfc_diff Main !! \ingroup Sfc_ex_cal !> \brief This is the first subroutine called in surface layer loop to @@ -132,8 +53,31 @@ end subroutine sfc_ex_coef_finalize !!| flag_iter | flag_for_iteration | flag for iteration | flag | 1 | logical | | in | F | !!| redrag | flag_for_reduced_drag_coefficient_over_sea | flag for reduced drag coefficient over sea | flag | 0 | logical | | in | F | !! -!! \section general_diff General Algorithm -!! +!> \section general_diff General Algorithm +!! -# Calculate the thermal roughness length formulation over the ocean (see eq. (25) and (26) +!! in Zeng et al.(1998) \cite zeng_et_al_1998). +!! -# Calculate Zeng's momentum roughness length formulation over land and sea ice. +!! -# Calculate the new vegetation-dependent formulation of thermal roughness length (Zheng et al. (2009) +!! \cite zheng_et_al_2009). +!! Zheng et al.(2009) \cite zheng_et_al_2009 proposed a new formulation on +!! \f$ln(Z_{0m}^,/Z_{0t})\f$ as follows: +!! \f[ +!! ln(Z_{0m}^,/Z_{0t})=(1-GVF)^2C_{zil}k(u*Z_{0g}/\nu)^{0.5} +!! \f] +!! where \f$Z_{0m}^,\f$ is the effective momentum roughness length +!! computed in the following equation for each grid, \f$Z_{0t}\f$ +!! is the roughness lenghth for heat, \f$C_{zil}\f$ is a coefficient +!! (taken as 0.8), k is the Von Karman constant (0.4), +!! \f$\nu=1.5\times10^{-5}m^{2}s^{-1}\f$ is the molecular viscosity, +!! \f$u*\f$ is the friction velocity, and \f$Z_{0g}\f$ is the bare +!! soil roughness length for momentum (taken as 0.01). +!! \n In order to consider the convergence of \f$Z_{0m}\f$ between +!! fully vegetated and bare soil, the effective \f$Z_{0m}^,\f$ is +!! computed: +!! \f[ +!! \ln(Z_{0m}^,)=(1-GVF)^{2}\ln(Z_{0g})+\left[1-(1-GVF)^{2}\right]\ln(Z_{0m}) +!!\f] +!! -# Calculate the exchange coefficients:\f$cm\f$, \f$ch\f$, and \f$stress\f$ as inputs of other \a sfc schemes. !! \section detailed_diff Detailed Algorithm !! !! @{ @@ -230,12 +174,14 @@ subroutine sfc_ex_coef_run & ! if(islimsk(i) == 0) then ! over ocean +! - Over the ocean, calculate friction velocity in eq.(A10) in Zeng et al. (1998) \cite zeng_et_al_1998 . ustar(i) = sqrt(grav * z0 / charnock) !** test xubin's new z0 ! ztmax = z0max +! - Over the ocean, calculate the roughness Reynolds number: restar = max(ustar(i)*z0max*visi, 0.000001) ! restar = log(restar) @@ -245,6 +191,8 @@ subroutine sfc_ex_coef_run & ! rat = rat / (1. + (bb2 + cc2*restar) * restar)) ! rat taken from zeng, zhao and dickinson 1997 +! - Over the ocean, calculate the roughness length of temperature +!! (see eq.(25) and (26) in Zeng et al. (1998) \cite zeng_et_al_1998). rat = min(7.0, 2.67 * sqrt(sqrt(restar)) - 2.57) ztmax = z0max * exp(-rat) @@ -255,7 +203,7 @@ subroutine sfc_ex_coef_run & tem1 = 1.0 - tem2 if( ivegsrc == 1 ) then - +! - Calculate the roughness length of momentum over land and sea ice. if (vegtype(i) == 10) then z0max = exp( tem2*log01 + tem1*log07 ) elseif (vegtype(i) == 6) then @@ -287,6 +235,8 @@ subroutine sfc_ex_coef_run & endif endif +! - Calculate the roughness length for heat (see eq.(1) of Zheng et al. (2012) +!! \cite zheng_et_al_2012 ) . z0max = max(z0max,1.0e-6) ! ! czilc = 10.0 ** (- (0.40/0.07) * z0) ! fei's canopy height dependance of czil @@ -408,6 +358,8 @@ subroutine sfc_ex_coef_run & ! ! finish the exchange coefficient computation to provide fm and fh ! +! - Finish the exchange coefficient computation to provide cm, ch, stress as input of other +! \a sfc schemes. fm(i) = fm(i) - pm fh(i) = fh(i) - ph fm10(i) = fm10(i) - pm10 diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index d0c40cdf2..043ea4437 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -1,8 +1,8 @@ !> \file sfc_drv.f -!! This file contains the NOAH land surface scheme driver. +!! This file contains the Noah land surface scheme driver. -!> \defgroup NOAH GFS NOAH Land Surface Scheme -!! \brief This it the NOAH Land Surface Model (NOAH LSM). +!> \defgroup NOAH GFS Noah Land Surface Scheme +!! \brief This it the Noah Land Surface Model (Noah LSM). !! !! Land-atmosphere interactions are a main driver of Earth's surface !! water and energy budgets. The importance of the land surface is @@ -33,12 +33,12 @@ !! small vertical dashed lines (no arrows) represent precipitation !! \image html Noah_LA_interaction.png "Figure 1: Local Land-atmosphere Interaction (courtesy of Micheal Ek, Ek and Mahrt (1994), Ek and Holtslag (2004))" width=10cm !! The land-surface model component was substantially upgraded from the Oregon -!! State University (OSU) land surface model to EMC's new NOAH Land Surface Model -!! (NOAH LSM) during the major implementation in the NCEP Global Forecast System -!! (GFS) on May 31, 2005. Forecast System (GFS). The NOAH LSM embodies about 10 +!! State University (OSU) land surface model to EMC's new Noah Land Surface Model +!! (Noah LSM) during the major implementation in the NCEP Global Forecast System +!! (GFS) on May 31, 2005. Forecast System (GFS). The Noah LSM embodies about 10 !! years of upgrades (see Chen et al. 1996 !! \cite chen_et_al_1996; Koren et al. 1999 \cite koren_et_al_1999; Ek et al. 2003 -!! \cite ek_et_al_2003) to its ancestor, the OSU LSM. The NOAH LSM upgrade includes: +!! \cite ek_et_al_2003) to its ancestor, the OSU LSM. The Noah LSM upgrade includes: !! - An increase from two (10, 190 cm thick) to four soil layers (10, !! 30, 60, 100 cm thick) !! - Addition of frozen soil physics @@ -59,7 +59,7 @@ !! !!\section Intraphysics Intraphysics Communication !! -! \defgroup NOAH_pre NOAH Land Surface Pre +! \defgroup NOAH_pre Noah Land Surface Pre ! \ingroup NOAH ! \brief Brief description of the parameterization ! @{ @@ -304,7 +304,7 @@ end subroutine lsm_noah_finalize !> \defgroup NOAH_drv GFS sfc_drv Main !! \ingroup NOAH !! @{ -!! \brief This is NOAH LSM driver scheme. +!! \brief This is Noah LSM driver scheme. !! !! \section arg_table_lsm_noah_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index 3f07e197f..5a9e7a96b 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -1,32 +1,6 @@ !> \file sfc_nst.f !! This file contains the GFS NSST model. -!> \defgroup GFS_NSST GFS Near Sea Surface Temperature -!! \brief Near Sea Surface Temperature (NSST) is a temperature profile just below the sea surface. The GFS NSST scheme is used to forecast the NSST for two main purposes: supply SSTs to the atmospheric model for the calculation of air-sea heat and moisture fluxes and providing a sub-layer temperature profile forecast for use as a first guess in the Gridpoint Statistical Interpolator (GSI) data assimilation code. -!! -!! The GFS NSST scheme was initially developed at NCEP by Xu Li in 2007, and subsequently received contributions by S. Moorthi, Y.-T. Hu and J. Derber, leading to operational implementation in the GFS in 2017 (Li 2015 \cite Li_2015, and Li and Derber 2009 \cite Li_Derber_2009). The GFS NSST scheme predicts the vertical profile of sea temperature between the surface and a reference level (zr), which is on the order of 5 m. Only two physical process are considered in this scheme: diurnal thermocline layer warming and thermal skin layer (also known as sub-layer) cooling. All other process that could influence NSST are ignored in this simple scheme. -!! -!!This profile is a composed by subdividing the near-surface layer in three parts -!! -!!T(z) = Tr + T’w (z) + T’c (z), -!! -!!where -!!Ts = T(z=0) is the SST -!!T’c (z) is the temperature profile in the skin layer (0 < z <= zc) -!!T’w (z) is the temperature profile in the warm layer (0 < z <= zr) -!!Tr is the reference temperature -!!zc is the depth of the skin layer -!! -!!Prediction for the skin layer is made using the Thermal Skin-layer Model (TSM), while prediction for the thermocline is based on the Diurnal Thermocline Model (DTM), both with an origin on Fairall et al. (1996) \cite Fairall_all_1996. Atmospheric inputs include short- and long-wave radiation, surface pressure, surface layer winds, temperature and specific humidity, and rainfall. -!! -!! \htmlonly -!! \endhtmlonly -!! @image html NSST.png "Figure 1: NSST profile." -!! -!! \section intraphysics_nst Intraphysics Communication -!! -!! This space is reserved for a description of how this scheme uses information from other scheme types and/or how information calculated in this scheme is used in other scheme types. - module sfc_nst contains @@ -46,6 +20,7 @@ end subroutine sfc_nst_init subroutine sfc_nst_finalize end subroutine sfc_nst_finalize +!> \defgroup GFS_NSST GFS Near Sea Surface Temperature !>\defgroup gfs_nst_main GFS sfc_nst Main !!\ingroup GFS_NSST !> \brief This is the second subroutine called in surface land loop. @@ -116,7 +91,7 @@ end subroutine sfc_nst_finalize !! !! This is the main subroutine for the NSST scheme, and it calls the DTM and TSM. !! -!! \section NSST_detailed_algorithm +!! \section NSST_detailed_algorithm Detailed Algorithm !! !! !> @{ @@ -711,8 +686,6 @@ module sfc_nst_pre !! !> \brief Brief description of the subroutine !! -!! Blah blah description of subroutine -!! !! \section arg_table_sfc_nst_init Argument Table !! subroutine sfc_nst_pre_init @@ -720,8 +693,6 @@ end subroutine sfc_nst_pre_init !> \brief Brief description of the subroutine !! -!! Blah blah description of subroutine -!! !! \section arg_table_sfc_nst_finalize Argument Table !! subroutine sfc_nst_pre_finalize diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 28c808f5a..5b44b8e06 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -1,54 +1,6 @@ !> \file sfc_sice.f !! This file contains the GFS three level thermodynamic sea ice model. -!> \defgroup GFS_Ice GFS Three-layer Thermodynamics Sea Ice -!! \brief This is three-layer thermodynomics sea-ice model based on Winton (2000) \cite winton_2000. -!! -!! Sea ice is a thin skin of frozen water covering the polar oceans. The sea ice strongly interacts with both the atmosphere above and the ocean underneath in the high -!! latitudes. In a coupled weather/climate system, changes in sea ice extent, thickness and concentration -!! regionally or globally would influence oceanic and atmospheric conditions, which in turn affect the -!! sea ice distribution. The physical and dynamical processes affecting the weather and climate are -!! considered as follows. -!! -!! The high albedo of the sea ice reflects more solar radiation back to the space. The feedbacks are -!! considered as positive. The broader the sea ice cover, the higher the surface albedo, which result -!! in less amount of solar radiation absorbed at the Earth's surface. A cooler surface would favor more -!! sea ice to form. The process would be reversed in less sea ice situation. -!! -!! The sea ice restricts the heat/water exchange between the air and ocean. The presence of extensive -!! areas of sea ice would suppress the heat loss in winter and the heat gain in summer by the ocean. -!! Even a thin ice cover influences the turbulent heat transfer significantly between ocean and -!! atmosphere. The surface fluxes of sensible and latent heat can be greater by up to two orders of magnitude -!! at the open water surface of a lead or polynya than that through (snow covered) pack ice. -!! -!! The sea ice modifies air/sea momentum transfer, ocean fresh water balance and ocean circulation. -!! The freezing and melting of the ocean surface and the associated fluxes of salt and heat produce major -!! changes in the density structure of the polar water. Formation of sea ice injects salt into the ocean -!! makes the water heavier and more convectively unstable, conversely when melting occurs, stable and fresh -!! layers can prevent deep covective activity. -!! -!! A sea ice model, in general, may contain subcomponents treating 1)dynamics (ice motion), -!! 2)ice transport, 3) multiple ice thickness categories (including leads), 4) surface albedo, -!! and 5) vertical thermodynamics. GFS sea ice scheme is concerned with a scheme for the -!! last of these processes. -!! -!! A three-layer thermodynamic sea ice model has been coupled to NCEP GFS. It predicts sea ice/snow thickness, -!! the surface temperature and ice temperature structure. In each model grid box, the heat and moisture -!! fluxes and albedo are treated separately for the ice and the open water. -!! -!!\image html GFS_sice_wonton2000_fig1.png "Fig.1 Schematic representation of the three-layer model" width=5cm -!! The model has four prognostic variables: the snow layer thickness \f$h_s\f$, the ice layer thickness -!! \f$h_i\f$, the upper and lower ice layer temperatures located at the midpoints of the layers -!! \f$h_i/4\f$ and \f$3h_i/4\f$ below the ice surface, respectively \f$T_1\f$ and \f$T_2\f$. The temperature of -!! the bottom of the ice is fixed at \f$T_f\f$, the freezing temperature of seawater. The temperature of -!! the top of the ice or snow, \f$T_s\f$, is determined from the surface energy balance. -!! -!! The model consists of a zero-heat-capacity snow layer overlying two equally thick sea ice layers (Fig.1). -!! The upper ice layer has a variable heat capacity to represent brine pockets. -!! -!! \section intraphysics_sice Intraphysics Communication -!!\image html schematic_sice.png "Fig.2 NCEP Sea Ice Model System Diagram" width=10cm - module sfc_sice contains @@ -66,8 +18,10 @@ subroutine sfc_sice_finalize end subroutine sfc_sice_finalize -!>\defgroup gfs_sice_main GFS sfc_sice Main +!> \defgroup GFS_Ice GFS Three-layer Thermodynamics Sea Ice !! @{ +!! \brief This is three-layer thermodynomics sea-ice model based on Winton (2000) \cite winton_2000. +!>\defgroup gfs_sice_main GFS sfc_sice Main !! \ingroup GFS_Ice !! \section arg_table_sfc_sice_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | @@ -114,8 +68,20 @@ end subroutine sfc_sice_finalize !! | hflx | kinematic_surface_upward_sensible_heat_flux | kinematic sensible heat flux | K m s-1 | 1 | real | kind_phys | out | F | !! !! \section general_sice_run General Algorithm +!! The ice model main program ice3lay() performs two functions: +!! - \b Calculation \b of \b ice \b temperature +!!\n The surface temperature is determined from the diagnostic balance between +!! the upward conduction of heat through snow and/or ice and upward flux of heat +!! from the surface. +!! +!! - \b Calculation \b of \b ice \b and \b snow \b changes +!!\n In addition to calculating ice temperature changes, the ice model must +!! also readjust the sizes of the snow and ice layers 1) to accommodate +!! mass fluxes at the upper and lower surfaces, 2) to convert snow below +!! the water line to ice, and 3) to equalize the thickness of the two +!! ice layers. !! \section detailed_sice_run Detailed Algorithm -!> @{ +!! @{ subroutine sfc_sice_run & & ( im, km, ps, u1, v1, t1, q1, delt, & & sfcemis, dlwflx, sfcnsw, sfcdsw, srflag, & @@ -217,13 +183,13 @@ subroutine sfc_sice_run & ! implicit none ! -! --- constant parameters: - integer, parameter :: kmi = 2 ! 2-layer of ice +! - Define constant parameters + integer, parameter :: kmi = 2 !> - 2-layer of ice real(kind=kind_phys), parameter :: cpinv = 1.0/cp real(kind=kind_phys), parameter :: hvapi = 1.0/hvap real(kind=kind_phys), parameter :: elocp = hvap/cp - real(kind=kind_phys), parameter :: himax = 8.0 ! maximum ice thickness allowed - real(kind=kind_phys), parameter :: himin = 0.1 ! minimum ice thickness required + real(kind=kind_phys), parameter :: himax = 8.0 !> - maximum ice thickness allowed + real(kind=kind_phys), parameter :: himin = 0.1 !> - minimum ice thickness required real(kind=kind_phys), parameter :: hsmax = 2.0 ! maximum snow depth allowed real(kind=kind_phys), parameter :: timin = 173.0 ! minimum temperature allowed for snow/ice real(kind=kind_phys), parameter :: albfw = 0.06 ! albedo for lead @@ -378,15 +344,17 @@ subroutine sfc_sice_run & snetw(i) = sfcdsw(i) * (1.0 - albfw) snetw(i) = min(3.0*sfcnsw(i)/(1.0+2.0*ffw(i)), snetw(i)) +! - Calculate sneti sneti(i) = (sfcnsw(i) - ffw(i)*snetw(i)) / fice(i) t12 = tice(i) * tice(i) t14 = t12 * t12 -! --- ... hfi = net non-solar and upir heat flux @ ice surface +! - Calculate hfi = net non-solar and upir heat flux @ ice surface hfi(i) = -dlwflx(i) + sfcemis(i)*sbc*t14 + evapi(i) & & + rch(i)*(tice(i) - theta1(i)) +! - Calculate hfd hfd(i) = 4.0*sfcemis(i)*sbc*tice(i)*t12 & & + (1.0 + elocp*eps*hvap*qs1/(rd*t12)) * rch(i) @@ -493,11 +461,28 @@ subroutine sfc_sice_run & contains ! ================= -!> @} !----------------------------------- !> This subroutine is the entity of three-layer sea ice vertical thermodynamics !! based on Winton(2000) \cite winton_2000 . +!! @{ +!!\ingroup gfs_sice_main +!!\param[in] im integer, horizontal dimension +!!\param[in] kmi integer, number of ice layers (2) +!!\param[in] fice real, sea-ice concentration +!!\param[in] flag logical, ice mask flag +!!\param[in] hfi real, net non-solar and heat flux at surface (\f$W/m^2\f$) +!!\param[in] hfd real, heat flux derivative at surface +!!\param[in] sneti real, net solar incoming at top (\f$W/m^2\f$) +!!\param[in] focn real, heat flux from ocean (\f$W/m^2\f$) +!!\param[in] delt real, time step(\f$sec\f$) +!!\param[in,out] snowd real, surface pressure +!!\param[in,out] hice real, sea-ice thickness +!!\param[in,out] stsice real, temperature at mid-point of ice levels (\f$^oC\f$) +!!\param[in,out] tice real, surface temperature (\f$^oC\f$) +!!\param[in,out] snof real, snowfall rate (\f$ms^{-1}\f$) +!!\param[out] snowmt real, snow melt during delt (\f$m\f$) +!!\param[out] gflux real, conductive heat flux (\f$W/m^2\f$) subroutine ice3lay !................................... ! --- inputs: @@ -758,6 +743,7 @@ subroutine ice3lay !................................... end subroutine ice3lay !----------------------------------- +!! @} ! =========================== ! ! end contain programs ! @@ -766,6 +752,8 @@ end subroutine ice3lay !................................... end subroutine sfc_sice_run !----------------------------------- +!! @} +!! @} end module sfc_sice @@ -773,14 +761,14 @@ module sfc_sice_pre contains -!! +! ! \brief This subroutine is empty since there are no procedures needed ! \section arg_table_sfc_sice_pre_init Argument Table ! subroutine sfc_sice_pre_init end subroutine sfc_sice_pre_init -!! +! ! \brief This subroutine is empty since there are no procedures needed ! \section arg_table_sfc_sice_pre_finalize Argument Table ! @@ -802,7 +790,6 @@ end subroutine sfc_sice_pre_finalize !! | tice | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kind_phys | out | F | !! | work3 | ratio_of_exner_function_between_midlayer_and_interface_at_lowest_model_layer | Exner function ratio bt midlayer and interface at 1st layer | ratio | 1 | real | kind_phys | out | F | !! -!! @{ subroutine sfc_sice_pre_run(im, fice, hice, tisfc , prsik, prslk, & & cice, zice, tice, work3) @@ -839,14 +826,14 @@ module sfc_sice_post contains -!! +! ! \brief This subroutine is empty since there are no procedures needed ! \section arg_table_sfc_sice_post_init Argument Table ! subroutine sfc_sice_post_init end subroutine sfc_sice_post_init -!! +! ! \brief This subroutine is empty since there are no procedures needed ! \section arg_table_sfc_sice_post_finalize Argument Table ! @@ -854,7 +841,7 @@ subroutine sfc_sice_post_finalize end subroutine sfc_sice_post_finalize -!! +! ! \section arg_table_sfc_sice_post_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|-------------------------------------------------------|---------------------------------------------|---------------|------|---------|-----------|--------|----------| @@ -868,7 +855,6 @@ end subroutine sfc_sice_post_finalize !! | hice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kind_phys | out | F | !! | tisfc | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kind_phys | out | F | !! -!! @{ subroutine sfc_sice_post_run(im, islmsk, cice, zice, tice, tsfc, & & fice, hice, tisfc) @@ -905,7 +891,5 @@ subroutine sfc_sice_post_run(im, islmsk, cice, zice, tice, tsfc, & enddo end subroutine sfc_sice_post_run -!! @} end module sfc_sice_post -!> @} From fdf93be4bc6c4b39eeb062b31b849177113b6ab5 Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Tue, 27 Feb 2018 16:51:01 -0700 Subject: [PATCH 16/22] more doxygen work are done. --- physics/docs/ccpp_dox | 14 +- physics/docs/library.bib | 114 +++++++- physics/docs/txt/GFS_GWDC.txt | 42 ++- physics/docs/txt/GFS_NOAH.txt | 41 ++- physics/docs/txt/GFS_NSST.txt | 6 +- physics/docs/txt/GFS_OZPHYS.txt | 61 ++++- physics/docs/txt/GFS_SFCLYR.txt | 2 +- physics/docs/txt/GFS_SFCSICE.txt | 2 +- physics/docs/txt/GFS_ZHAOC.txt | 18 +- physics/docs/txt/mainpage_bootstrapped.txt | 2 - physics/gscond.f | 21 +- physics/gwdc.f | 90 ++++--- physics/mfdeepcnv.f | 2 - physics/mfshalcnv.f | 187 ++++++------- physics/module_nst_model.f90 | 17 +- physics/module_nst_parameters.f90 | 67 ++--- physics/module_nst_water_prop.f90 | 2 +- physics/ozphys.f | 24 +- physics/radlw_main.f | 2 +- physics/sfc_diff.f | 2 +- physics/sfc_drv.f | 210 ++++++--------- physics/sfc_nst.f | 64 +++-- physics/sfc_sice.f | 296 ++++++++++----------- physics/sfcsub.f | 4 +- physics/sflx.f | 282 ++++++++++++++------ 25 files changed, 900 insertions(+), 672 deletions(-) diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index b0a5f8b2a..a93ba6d43 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -1,7 +1,7 @@ # Doxyfile 1.8.11 DOXYFILE_ENCODING = UTF-8 -PROJECT_NAME = "GMTB Common Community Physics Package(CCPP) Documentation" -PROJECT_NUMBER = "Version 0" +PROJECT_NAME = "GMTB Common Community Physics Package (CCPP) Documentation" +PROJECT_NUMBER = "Version 1" PROJECT_BRIEF = "" PROJECT_LOGO = img/dtc_logo.png OUTPUT_DIRECTORY = doc @@ -112,8 +112,6 @@ INPUT = txt/mainpage_bootstrapped.txt \ txt/GFS_GWDPS.txt \ txt/GFS_GWDC.txt \ txt/GFS_OZPHYS.txt \ - txt/GFS_CALPRECIPTYPE.txt \ - txt/GFS_RAYLEIGH.txt \ ### Radiation ../radiation_aerosols.f \ ../radiation_astronomy.f \ @@ -141,10 +139,7 @@ INPUT = txt/mainpage_bootstrapped.txt \ ### Land Surface ../sfc_drv.f \ ../sflx.f \ - ../sfcsub.f \ ../sfc_diff.f \ - ../set_soilveg.f \ - ../GFS_calpreciptype.f90 \ ### Sea Ice Surface ../sfc_sice.f \ ### Ocean Surface @@ -156,10 +151,9 @@ INPUT = txt/mainpage_bootstrapped.txt \ ../gwdps.f \ ### Convective Gravity Wave ../gwdc.f \ -### Rayleigh damp - ../rayleigh_damp.f \ ### Prognostic Ozone - ../ozphys.f + ../ozinterp.f90 \ + ../ozphys.f \ INPUT_ENCODING = UTF-8 FILE_PATTERNS = *.f \ *.txt diff --git a/physics/docs/library.bib b/physics/docs/library.bib index 7f7fcf3c0..2f99a8efd 100644 --- a/physics/docs/library.bib +++ b/physics/docs/library.bib @@ -1,19 +1,123 @@ %% This BibTeX bibliography file was created using BibDesk. %% http://bibdesk.sourceforge.net/ -%% Created for Man Zhang at 2018-02-14 15:01:01 -0700 +%% Created for Man Zhang at 2018-02-26 15:56:22 -0700 %% Saved with string encoding Unicode (UTF-8) +@article{dethof_and_holm_2004, + Author = {A. Dethof and E. V. Holm}, + Date-Added = {2018-02-26 22:54:54 +0000}, + Date-Modified = {2018-02-26 22:56:19 +0000}, + Journal = {Quarterly Journal of the Royal Meteorological Society}, + Pages = {2851-2872}, + Title = {Ozone assimilation in the ERA-40 reanalysis project}, + Volume = {130}, + Year = {2004}} + +@techreport{jackson_and_saunders_2002, + Author = {D. R. Jackson and R. Saunders}, + Date-Added = {2018-02-26 22:46:33 +0000}, + Date-Modified = {2018-02-26 22:49:04 +0000}, + Institution = {Met Office}, + Number = {394}, + Title = {Ozone data assimilation: preliminary system}, + Type = {Forecasting Research Technical Report }, + Year = {2002}} + +@article{riishojgaard_1996, + Author = {L. P. Riishojgaard}, + Date-Added = {2018-02-26 22:43:38 +0000}, + Date-Modified = {2018-02-26 22:45:36 +0000}, + Journal = {Quarterly Journal of the Royal Meteorological Society}, + Pages = {1545-1571}, + Title = {On four-dimensional variational assimilation of ozone data in weather-prediction models}, + Volume = {122}, + Year = {1996}} + +@article{john_and_buehler_2004, + Author = {V. O. John and S. A. Buehler}, + Date-Added = {2018-02-26 22:38:57 +0000}, + Date-Modified = {2018-02-26 22:41:05 +0000}, + Journal = {Geophysical Research Letters}, + Title = {The impact of ozone lines on AMSU-B radiances}, + Volume = {31}, + Year = {2004}} + +@article{derber_and_wu_1998, + Author = {J. C. Derber and W.-S. Wu}, + Date-Added = {2018-02-26 22:35:19 +0000}, + Date-Modified = {2018-02-26 22:37:30 +0000}, + Journal = {Monthly Weather Review}, + Pages = {2287-2299}, + Title = {The use of TOVS cloud-cleared radiances in the NCEP SSI analysis system}, + Volume = {126}, + Year = {1998}} + +@inbook{hooke_1986, + Author = {W.H. Hooke}, + Chapter = {Gravity Waves}, + Date-Added = {2018-02-23 17:06:35 +0000}, + Date-Modified = {2018-02-23 17:10:25 +0000}, + Editor = {P. S. Ray}, + Number = {12}, + Pages = {272-288}, + Publisher = {American Meteorological Society}, + Title = {Mesoscale meteorology and forecasting}, + Year = {1986}} + +@article{kim_et_al_2003, + Author = {Y.-J. Kim and S. D. Eckermann and H.-Y. Chun}, + Date-Added = {2018-02-23 16:59:17 +0000}, + Date-Modified = {2018-02-23 17:02:12 +0000}, + Journal = {Atmosphere-Ocean}, + Number = {1}, + Pages = {65-98}, + Title = {An overview of the past, present and future of gravity-wave drag parameterization for numerical climate and weather prediction models}, + Volume = {41}, + Year = {2003}} + +@article{paulson_and_simpson_1981, + Author = {C.A. Paulson and J.J. Simpson}, + Date-Added = {2018-02-21 23:47:11 +0000}, + Date-Modified = {2018-02-21 23:50:29 +0000}, + Journal = {J. Geophys. Res.}, + Number = {C11}, + Pages = {2156-2202}, + Title = {The temperature difference across the cool skin of the ocean}, + Volume = {86}, + Year = {1981}} + +@article{peters-lidard_et_al_1997, + Author = {C. D. Peters-Lidard and M. S. Zion and E. F. Wood}, + Date-Added = {2018-02-20 19:44:29 +0000}, + Date-Modified = {2018-02-20 19:46:55 +0000}, + Journal = {J. Geophys. Res.}, + Number = {D4}, + Pages = {4303-4324}, + Title = {A soil-vegetation-atmosphere transfer sheme for modeling spatially variable water and energy balance processes}, + Volume = {102}, + Year = {1997}} + +@article{peters-lidard_et_al_1998, + Author = {C. D. Peters-Lidard and E. Blackburn and X. Liang and E. F. Wood}, + Date-Added = {2018-02-20 19:28:47 +0000}, + Date-Modified = {2018-02-20 19:31:50 +0000}, + Journal = {J. Atmos. Sci.}, + Pages = {1209-1224}, + Title = {The effect of soil thermal conductivity parameterization on surface energy fluxes and temperatures}, + Volume = {55}, + Year = {1998}} + @book{pond_and_pickard_1983, Author = {S. Pond and G.L. Pickard}, Date-Added = {2018-02-14 21:57:02 +0000}, Date-Modified = {2018-02-14 22:00:44 +0000}, Edition = {2nd}, - Publisher = {Pergamon Press }, + Publisher = {Pergamon Press}, Title = {Introductory dynamical oceanography}, Year = {1983}} @@ -352,8 +456,9 @@ @url{Li_Derber_2009 Url = {https://www.jcsda.noaa.gov/documents/meetings/wkshp2008/4/JCSDA_2008_Li.pdf}, Bdsk-Url-1 = {https://www.jcsda.noaa.gov/documents/meetings/wkshp2008/4/JCSDA_2008_Li.pdf}} -@article{Fairall_all_1996, +@article{Fairall_et_al_1996, Author = {C. W. Fairall and E. F. Bradley and J. S. Godfrey and G. A. Wick and J. B. Edson and G. S. Young}, + Date-Modified = {2018-02-21 22:01:48 +0000}, Journal = {J. Geophys. Res.}, Pages = {1295-1308}, Title = {Cool-skin and warm-layer effects on sea surface temperature}, @@ -1065,9 +1170,8 @@ @techreport{chou_and_suarez_1999 @article{sato_et_al_1993, Author = {M. Sato and J.E. Hansan and M. P. McCormick and J. B. Pollack}, Date-Added = {2016-05-20 04:23:08 +0000}, - Date-Modified = {2016-05-20 15:07:03 +0000}, + Date-Modified = {2018-02-20 19:58:29 +0000}, Journal = {J. Geophys. Res.}, - Month = {December}, Number = {D12}, Pages = {22987-22994}, Title = {Stratospheric aerosol optical depth, 1985-1990}, diff --git a/physics/docs/txt/GFS_GWDC.txt b/physics/docs/txt/GFS_GWDC.txt index 7982f167a..128c95dd0 100644 --- a/physics/docs/txt/GFS_GWDC.txt +++ b/physics/docs/txt/GFS_GWDC.txt @@ -3,10 +3,13 @@ \section des_gwdc 1. Description GFS physics includes parameterizations of gravity waves from two important sources: mountains and convection. This parameterization - addresses the latter. + addresses the latter. - In a review paper on gravity waves in the middle atmosphere, Fritts - (1984) \cite fritts_1984 showed that a large portion of observed + The importance of convectively-generated tropical waves + in driving the equatorial stratospheric semi-annual oscillation (SAO) and + quasi-biennial oscillation (QBO) has been appreciated for many years. + In a review paper on gravity waves in the middle atmosphere, Fritts (1984) \cite fritts_1984 + showed that a large portion of observed gravity wave momentum flux has higher frequencies than those of stationary mountain waves. This phenomenon was explained by cumulus convection, which is an additional source of tropospheric gravity @@ -21,26 +24,19 @@ the stable stratosphere can generate gravity waves that influence the large-scale flow. - Parameterizing subgrid-scale convection-induced gravity wave - momentum flux for use in large-scale models inherently requires - some information from subgrid-scale cumulus parameterization. - The methodology for parameterizing the zonal momentum flux induced - by thermal forcing can be summarized as follows. From the cloud-base - to cloud-top height, the effect of the momentum flux - induced by subgrid-scale diabatic forcing is not considered because - subgrid-scale cumulus convection in large-scale models is only - activated in a conditionally unstable atmosphere. Below the cloud - base, the momentum flux is also not considered because of the wave - momentum cancellation. At the cloud top, the momentum flux is - obtained by eq.(18) and (19) in Chun and Baik (1998) - \cite chun_and_baik_1998. Above the cloud top, there are two ways to - construct the momentum flux profile. One way is to specify a - vertical structure of the momentum flux normalized by the cloud-top - value, similar to what has been done for mountain drag - parameterization. The other way is to apply the wave saturation - hypothesis in order to find wave breaking levels in terms of the - Richardon number criterion using the nonlinearity factor of - thermally induced waves. + \image html GFS_gwdc.png "Figure 1: Gravity waves generated by penetrative convection in the presence of background wind. (Based on Hooke(1986) \cite hooke_1986; and Kim et al. (2003) \cite kim_et_al_2003)" width=10cm + + Compared with orographic gravitity waves, it has proven more difficult to model the way in which + gravity waves are generated by various convective sources; The simplest situation is depicted in + Fig.1. There are several proposed generation mechanisms in the literature (see section 3b in + Kim et al. (2003) \cite kim_et_al_2003).Amongst, Chun and Baik (1998) \cite chun_and_baik_1998 + proposed a way for parameterizing + convection-induced subgrid-scale gravity wave momentum flux in large-scale models. + For the momentum flux profile up to the cloud-top height, use of the linear + analytical form was suggested. In GFS operaional physics suite, the effect + of convection-induced gravity wave momentum flux is included + only above the cloud-top height because subgrid-scale cumulus parameterization + is activated in a conditionally unstable atmosphere. \section intra_gwdc 2. Intraphysics Communication \sa \ref arg_table_gwdc_run diff --git a/physics/docs/txt/GFS_NOAH.txt b/physics/docs/txt/GFS_NOAH.txt index 547898075..6e47d6bc1 100644 --- a/physics/docs/txt/GFS_NOAH.txt +++ b/physics/docs/txt/GFS_NOAH.txt @@ -1,5 +1,5 @@ /** -\page GFS_NOAH GFS Noah Land Surface Scheme +\page GFS_NOAH GFS Noah Land Surface Model \section des_noah 1. Description Land-atmosphere interactions are a main driver of Earth's surface water and energy budgets. The importance of the land surface is @@ -28,34 +28,31 @@ with arrows also represent positive feedbacks. The single horizontal gay-dotted line (no arrows) indicates the top of the PBL, and the seven small vertical dashed lines (no arrows) represent precipitation - \image html Noah_LA_interaction.png "Figure 1: Local Land-atmosphere Interaction (courtesy of Micheal Ek, Ek and Mahrt (1994), Ek and Holtslag (2004))" width=10cm - The land-surface model component was substantially upgraded from the Oregon - State University (OSU) land surface model to EMC's new NOAH Land Surface Model - (NOAH LSM) during the major implementation in the NCEP Global Forecast System - (GFS) on May 31, 2005. Forecast System (GFS). The NOAH LSM embodies about 10 - years of upgrades (see Chen et al. 1996 - \cite chen_et_al_1996; Koren et al. 1999 \cite koren_et_al_1999; Ek et al. 2003 - \cite ek_et_al_2003) to its ancestor, the OSU LSM. The NOAH LSM upgrade includes: - - An increase from two (10, 190 cm thick) to four soil layers (10, 30, 60, 100 cm thick) - - Addition of frozen soil physics - - Add glacial ice treatment - - Two snowpack states (SWE, density) - - New formulations for infiltration and runoff account for sub-grid variability in precipitation and soil moisture - - Revised physics of the snowpack and its influence on surface heat fluxes and albedo - - Higher canopy resistance - - Spatially varying root depth - - Surface fluxes weighted by snow cover fraction - - Improved thermal conduction in soil/snow - - Improved seasonality of green vegetation cover. - - Improved evaporation treatment over bare soil and snowpack + \image html Noah_LA_interaction.png "Figure 1: Local Land-atmosphere Interaction (courtesy of Michael Ek, Ek and Mahrt (1994), Ek and Holtslag (2004))" width=10cm + +Recently, the land surface updates in 2017 GFS operational physics includes: + - IGBP 20-type 1-km land classification + - STASGO 19-type 1-km soil classification + - MODIS-based snow free albedo + - MODIS-based maximum snow albedo + - Diurnal albedo treatment + - Unify snow cover, albedo between radiation and land surface model + - Increase ground heat flux under deep snow + - Upgrade surface layer parameterization scheme \ref GFS_SFCLYR to modify the roughness-length formulation and introduce a stability parameter constraint in the Monin-Obukhov similarity theory to prevent the land-atmosphere system from fully decoupling leading to excessive cooling of 2m temperature during sunset \image html land_dataset.png "Figure 2: Land Data Sets Used in NCEP Modeling Systems" width=10cm +This scheme include the following modules: + + \ref Noah_drv + + \ref Noah_LSM \section intra_noah 2. Intraphysics Communication -\ref arg_table_lsm_noah_run + + GFS Noah LSM Driver (\ref arg_table_lsm_Noah_run) + + GFS Noah LSM Model (sflx()) \section gen_al_noah 3. General Algorithm ++ GFS Noah LSM Driver (\ref general_noah_drv) ++ GFS Noah LSM Model (\ref general_sflx) diff --git a/physics/docs/txt/GFS_NSST.txt b/physics/docs/txt/GFS_NSST.txt index 7cdc4d336..ab255f262 100644 --- a/physics/docs/txt/GFS_NSST.txt +++ b/physics/docs/txt/GFS_NSST.txt @@ -16,7 +16,7 @@ where \n Tr is the reference temperature \n zc is the depth of the skin layer -Prediction for the skin layer is made using the Thermal Skin-layer Model (TSM), while prediction for the thermocline is based on the Diurnal Thermocline Model (DTM \ref nst_module), both with an origin on Fairall et al. (1996) \cite Fairall_all_1996. Atmospheric inputs include short- and long-wave radiation, surface pressure, surface layer winds, temperature and specific humidity, and rainfall. +Prediction for the skin layer is made using the Thermal Skin-layer Model (TSM), while prediction for the thermocline is based on the Diurnal Thermocline Model (DTM), both with an origin on Fairall et al. (1996) \cite fairall_et_al_1996. Atmospheric inputs include short- and long-wave radiation, surface pressure, surface layer winds, temperature and specific humidity, and rainfall. @image html NSST.png "Figure 1: NSST profile." @@ -32,9 +32,5 @@ This scheme includes the following components: \section gen_nst 3. General Algorithm \sa \ref NSST_general_algorithm -\section det_nst 4. Detailed Algorithm -\sa \ref NSST_detailed_algorithm - - */ diff --git a/physics/docs/txt/GFS_OZPHYS.txt b/physics/docs/txt/GFS_OZPHYS.txt index e117e61ee..2ae0c5ec9 100644 --- a/physics/docs/txt/GFS_OZPHYS.txt +++ b/physics/docs/txt/GFS_OZPHYS.txt @@ -1,20 +1,59 @@ /** -\page GFS_OZPHYS GFS Ozone Sources and Sinks Scheme +\page GFS_OZPHYS GFS Ozone Physics \section des_ozone 1. Description - The operational GFS currently parameterizes ozone production and - destruction based on monthly mean coefficients provided by Naval - Research Laboratory through CHEM2D chemistry model - (McCormack et al. 2006 \cite mccormack_et_al_2006). - Monthly and zonal mean ozone production rate and ozone destruction - rate per unit ozone mixing ratio were provided by NRL based on - CHEM2D model. - Original version of these terms were provided by NASA/DAO based on - NASA 2D Chemistry model - GSM is capable of running both versions + In recent years, the leading NWP centers have extended the vertical range of their NWP and DA systems + from the surface up through the stratosphere (~10-50 km altitude) and lower mesosphere (~50-65 km). Some + have also added stratospheric ozone (\f$O_3\f$) as a prognostic trace constituent to their models. Examples + include the Integrated Forecast System (IFS) of the European Centre for Medium Range Weather Forecasts (ECMWF)(Untch et al., 1999\cite untch_et_al; Dethof and Holm, 2004 \cite dethof_and_holm_2004), and the NCEP GFS (NCEP 2003). The addition + of stratospheric ozone as a prognostic variable is expected to improve overall forecast and analyses skill of other fields, + such as temperature and wind. The primary reasons for this are: + - more accurate assimilation of satellite radiances from channels that are sensitive to ozone(Derber and Wu, 1998 \cite derber_and_wu_1998; John and Buehler, 2004 \cite john_and_buehler_2004); + - utilization of correlations between ozone and wind to improve wind analyses in the upper troposphere and lower stratosphere +(UTLS) (e.g. Riishojgaard, 1996 \cite riishojgaard_1996); + - more accurate radiative heating rates, and hence temperatures arising from using analysed ozone rather than climatological +ozone in the forecast model radiation sheme (often referred to as 'ozone/radiation interaction') (Jackson and Saunders, 2002 \cite jackson_and_saunders_2002); + - more accurate analyses and forecasts of surface ultraviolet (UV) radiation. + + With the extension of NWP/DA systems into the upper stratosphere, assimilation and advection alone cannot yield accurate ozone + forecasts - photochemical effects must also be included. Due to the complexity of ozone photochemistry, it is not currently + feasible to implement full ozone photochemistry within a high-resolution operational global NWP system. Instead, + the operational GFS currently parameterizes photochemical production and destruction based on + monthly mean coefficients provided by Naval Research Laboratory CHEM2D chemistry model through an ozone photochemistry parameterization (OPP), + known as CHEM2D-OPP (McCormack et al. 2006 \cite mccormack_et_al_2006). CHEM2D-OPP consists of four coefficients describing + the residual ozone photochemical tendency as the difference between the production and loss rates \f$(P-L)\f$ + and its sensitivity to local changes in ozone mixing ratio \f$r\f$, temperature \f$T\f$, and overhead ozone column amount \f$\Sigma\f$ (see Figs. 1, 2, + 5, and 6 in McCormack et al. 2006 \cite mccormack_et_al_2006). The local time rate of change of ozone mixing ratio due to + photochemistry is then: + \f[ + \frac{\partial r}{\partial t}=(P-L)\left[r,T,\Sigma\right] + \color{red} {(1)} + \f] + + Linearization of the ozone photochemical tendency above has become a standard method for NWP and climate models. The latest + generation of linearized ozone photochemistry scheme approximate the unknown function \f$(P-L)\left[r,T,\Sigma\right]\f$ by + defining it about some reference state \f$r_0\f$,\f$T_0\f$,\f$\Sigma_0\f$, then expanding it about this reference state + using a first-order Taylor series expansion. + \f[ + \frac{\partial r(\lambda,\phi,p,t)}{\partial t}=(P-L)_0+\frac{\partial (P-L)}{\partial r}\bracevert_0(r-r_0)+\frac{\partial (P-L)}{\partial T}\bracevert_0(T-T_0)+\frac{\partial (P-L)}{\partial \Sigma}\bracevert_0(\Sigma-\Sigma_{0}) + \color{red} {(2)} + \f] + where \f$\lambda\f$ represents longtitude, \f$\phi\f$ represents latitude, and \f$p\f$ represents pressure as the model + vertical coordinate. The subscript "0" attached to \f$(P-L)\f$ and its partial derivatives refers to their values + at the reference state \f$r_0\f$,\f$T_0\f$,\f$\Sigma_0\f$, and are all zonally averaged quantities. + The reference-state production and loss, \f$(P-L)_0\f$, and the various partial derivative terms about the state (the last + three terms on the right) are computed offline using CHEM2D model photochemistry. These coefficients are then stored in tabular + form as functions of latitude, pressure, and month, with suitable linear interpolation to the desired location (\c global_o3prdlos.f77). + However, when implementing (2) in GFS physics suite, the perturbation terms \f$(r-r_0, T-T_0, \Sigma-\Sigma_0)\f$ are computed + with respect to a zonal mean climatological reference state used to derive the partial derivatives in (2). such discrepancies + can potentially introduce systematic, non-physical biases into the photochemical parameterization (McCormack et al. 2006 \cite mccormack_et_al_2006). + + \section intra_ozone 2. Intraphysics Communication -\ref arg_table_ozphys_run +\sa \ref arg_table_ozphys_run \section gen_ozone 3. General Algorithm +\sa \ref genal_ozphys diff --git a/physics/docs/txt/GFS_SFCLYR.txt b/physics/docs/txt/GFS_SFCLYR.txt index 20a20e174..7daae3adf 100644 --- a/physics/docs/txt/GFS_SFCLYR.txt +++ b/physics/docs/txt/GFS_SFCLYR.txt @@ -1,5 +1,5 @@ /** -\page GFS_SFCLYR GFS Surface Sublayer Scheme +\page GFS_SFCLYR GFS Surface Layer Scheme \section des_rough 1. Description It is the surface roughness length calculation based on the surface sublayer scheme from Zeng and Dickinson (1998) diff --git a/physics/docs/txt/GFS_SFCSICE.txt b/physics/docs/txt/GFS_SFCSICE.txt index 19eebddc9..d6fdf64b6 100644 --- a/physics/docs/txt/GFS_SFCSICE.txt +++ b/physics/docs/txt/GFS_SFCSICE.txt @@ -1,7 +1,7 @@ /** \page GFS_SFCSICE GFS Sea Ice Scheme \section des_sice 1. Description - This is three-layer thermodynomics sea-ice model based on Winton (2000) \cite winton_2000. + This is the three-layer thermodynomics sea-ice model based on Winton (2000) \cite winton_2000. Sea ice is a thin skin of frozen water covering the polar oceans. The sea ice strongly interacts with both the atmosphere above and the ocean underneath in the high diff --git a/physics/docs/txt/GFS_ZHAOC.txt b/physics/docs/txt/GFS_ZHAOC.txt index 8fdd58bd8..80bc402b8 100644 --- a/physics/docs/txt/GFS_ZHAOC.txt +++ b/physics/docs/txt/GFS_ZHAOC.txt @@ -60,22 +60,16 @@ \cite heymsfield_and_mcfarquhar_1996) was introduced. \section intro_zhao 2. Intraphysics Communication - + For grid-scale condensation and evaporation of cloud process - \sa \ref arg_table_gscond_run - + For precipitation (snow or rain) production - \sa \ref arg_table_precpd_run + + For grid-scale condensation and evaporation of cloud process: \ref arg_table_gscond_run + + For precipitation (snow or rain) production: \ref arg_table_precpd_run \section Gen_zhao 3. General Algorithm - + For grid-scale condensation and evaporation of cloud process - \sa \ref general_gscond - + For precipitation (snow or rain) production - \sa \ref general_precpd + + For grid-scale condensation and evaporation of cloud process: \ref general_gscond + + For precipitation (snow or rain) production: \ref general_precpd \section det_zhao 4. Detailed Algorithm - + For grid-scale condensation and evaporation of cloud process - \sa \ref Zhao-Carr_cond_detailed - + For precipitation (snow or rain) production - \sa \ref Zhao-Carr_precip_detailed + + For grid-scale condensation and evaporation of cloud process: \ref Zhao-Carr_cond_detailed + + For precipitation (snow or rain) production: \ref Zhao-Carr_precip_detailed diff --git a/physics/docs/txt/mainpage_bootstrapped.txt b/physics/docs/txt/mainpage_bootstrapped.txt index 129e42b99..883304d94 100644 --- a/physics/docs/txt/mainpage_bootstrapped.txt +++ b/physics/docs/txt/mainpage_bootstrapped.txt @@ -23,8 +23,6 @@ Documentation for the individual physics scheme can of 2017 operational GFS phys + @ref GFS_GWDPS + @ref GFS_GWDC + @ref GFS_OZPHYS - + @ref GFS_CALPRECIPTYPE - + @ref GFS_RAYLEIGH You can find more information about GMTB Interoperable Physics Driver/Common Community Physics Package(IPD/CCPP) on DTC website diff --git a/physics/gscond.f b/physics/gscond.f index 2502fb653..638c94a6a 100644 --- a/physics/gscond.f +++ b/physics/gscond.f @@ -6,9 +6,6 @@ module GFS_zhaocarr_gscond contains -!> \defgroup Zhao-Carr GFS Zhao-Carr Microphysics -!! @{ -!! ! \brief Brief description of the subroutine ! @@ -17,6 +14,17 @@ module GFS_zhaocarr_gscond subroutine gscond_init end subroutine gscond_init +! \brief Brief description of the subroutine +! +! \section arg_table_gscond_finalize Argument Table +! + subroutine gscond_finalize + end subroutine gscond_finalize + + +!> \defgroup Zhao-Carr GFS Zhao-Carr Microphysics +!! @{ +!! !> \defgroup condense Grid-Scale Condensation and Evaporation of Cloud !! @{ !! \brief This subroutine computes grid-scale condensation and evaporation of @@ -504,13 +512,6 @@ end subroutine gscond_run !> @} !! @} -! \brief Brief description of the subroutine -! -! \section arg_table_gscond_finalize Argument Table -! - subroutine gscond_finalize - end subroutine gscond_finalize - !! @} diff --git a/physics/gwdc.f b/physics/gwdc.f index 4161179c4..7953220d5 100644 --- a/physics/gwdc.f +++ b/physics/gwdc.f @@ -148,7 +148,27 @@ end subroutine gwdc_init !! | taucty | instantaneous_y_stress_due_to_gravity_wave_drag | meridional stress at cloud top due to convective gravity wave drag | Pa | 1 | real | kind_phys | out | F | !! !> \section gen_gwdc General Algorithm +!! Parameterizing subgrid-scale convection-induced gravity wave +!! momentum flux for use in large-scale models inherently requires +!! some information from subgrid-scale cumulus parameterization. +!! The methodology for parameterizing the zonal momentum flux induced +!! by thermal forcing can be summarized as follows. From the cloud-base +!! to cloud-top height, the effect of the momentum flux +!! induced by subgrid-scale diabatic forcing is not considered because +!! subgrid-scale cumulus convection in large-scale models is only +!! activated in a conditionally unstable atmosphere. Below the cloud +!! base, the momentum flux is also not considered because of the wave +!! momentum cancellation. !! +!! The formulation of the momentum flux at the cloud top that can be broken +!! in the upper atmosphere is similar to that of the surface drag of mountain +!! waves by using the nonlinearity factor of thermally induced waves that is +!! analogous to the inverse Frounde number in mountain waves. A vertical +!! profiles of redistributed momentum flux above the cloud top can be approximated +!! either by specifying a functional form or by using the wave saturation hypothesis +!! in terms of the Richardson number criterion. The formulation of the minimum +!! Richardson number including wave impact is similar to that in the mountain +!! wave case. !> \section al_gwdc Detailed Algorithm !> @{ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & @@ -341,6 +361,7 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & &, riminp=-0.99e+20, rismall=-0.9e+20 ! +!> - Determine if deep convection occurs and activate convection-induced GWD scheme. npt = 0 do i = 1,im ipt(i) = 0 @@ -442,8 +463,8 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & & brunm(npt,km), rhom(npt,km)) !----------------------------------------------------------------------- -!> -# Create local arrays with reversed vertical indices -!! and Initialize local variables +!> - Create local arrays with reversed vertical indices +!! and Initialize local variables. !----------------------------------------------------------------------- gsqr = grav * grav onebg = one / grav @@ -685,9 +706,9 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & !----------------------------------------------------------------------- ! -!> -# Calculate the cloud top wind components and speed. -!! Here, ucltop, vcltop, and windcltop are wind components and -!! wind speed at mid-level cloud top index +!> - Calculate the cloud top wind components, speed and direction. +! Here, ucltop, vcltop, and windcltop are wind components and +! wind speed at mid-level cloud top index ! !----------------------------------------------------------------------- @@ -703,12 +724,12 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & !----------------------------------------------------------------------- ! -!> -# Calculate the basic state wind projected in the direction of the -!! cloud top wind at mid level and interface level (U, UI), where: -!! \n U : Basic-wind speed profile. Basic-wind is parallel to the wind -!! vector at the cloud top level. (mid level) -!! \n UI: Basic-wind speed profile. Basic-wind is parallel to the wind -!! vector at the cloud top level. ( interface level ) +!> - Calculate the basic state wind profiles projected in the direction of the +!! cloud top wind at mid level and interface level. +! \n U : Basic-wind speed profile. Basic-wind is parallel to the wind +! vector at the cloud top level. (mid level) +! \n UI: Basic-wind speed profile. Basic-wind is parallel to the wind +! vector at the cloud top level. ( interface level ) ! Input u(i,k) and v(i,k) is defined at mid level ! !----------------------------------------------------------------------- @@ -743,7 +764,7 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & !----------------------------------------------------------------------- ! -!> -# Calculate the local Richardson number +!> - Calculate the local Richardson number: !! \f[ !! Ri=N^2/\eta^2 !! \f] @@ -811,7 +832,7 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & !----------------------------------------------------------------------- ! -!> -# Calculate the gravity wave stress at the interface level cloud top. +!> - Calculate the gravity wave stress at the interface level cloud top. ! ! kcldtopi : The interface level cloud top index ! kcldtop : The midlevel cloud top index @@ -852,11 +873,17 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & ! GWDC calculation in current horizontal grid is skipped. ! ! G : If mean wind at the cloud top is less than zero, GWDC - +! calculation in current horizontal grid is skipped. +! +!----------------------------------------------------------------------- +!D !> - Wave stress at cloud top is calculated when the atmosphere -!! is dynamically stable at the cloud top -!! -!> - The cloud top wave stress and nonlinear parameter are calculated +!! is dynamically stable at the cloud top. + do i=1,npt + kk = kcldtop(i) + if ( abs(basicui(i,kk)) > zero .and. riloc(i,kk) > ricrit) then +!E +!> - The cloud top wave stress and nonlinear parameter are calculated !! using density, temperature, and wind that are defined at mid !! level just below the interface level in which cloud top wave !! stress is defined. @@ -887,20 +914,7 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & !! top heights of thermal forcing. If the atmosphere is dynamically !! unstable at the cloud top, the convective GWD calculation is !! skipped at that grid point. -!! -! - If mean wind at the cloud top is less than zero, GWDC -! calculation in current horizontal grid is skipped. -! -!> - The stress is capped at tauctmax = - 5\f$n/m^2\f$ -!! in order to prevent numerical instability. -! -!----------------------------------------------------------------------- -!D - do i=1,npt - kk = kcldtop(i) - if ( abs(basicui(i,kk)) > zero .and. riloc(i,kk) > ricrit) then -!E tem = basicum(i,kk) tem1 = tem * tem nonlinct = gqmcldlen(i) / (bruni(i,kk)*t(i,kk)*tem1) ! Mu @@ -908,6 +922,8 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & ! RhoU^3c1(c2mu)^2/Ndx tauct = - rhom(i,kk) * tem * tem1 * c1 * tem2 * tem2 & / (bruni(i,kk)*dlen(i)) +!> - The stress is capped at \f$\tau_{x} = - 5n/m^2\f$ +!! in order to prevent numerical instability. tauct = max(tauctmax, tauct) tauctxl(i) = tauct * cosphi(i) ! X stress at cloud top @@ -916,6 +932,12 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & do_gwc(i) = .true. else !F +!> - If the atmosphere is dynamically unstable at the cloud top, +!! GWDC calculation in current horizontal grid is skipped. +!> - If mean wind at the cloud top is less than zero, GWDC +!! calculation in current horizontal grid is skipped. + + tauctxl(i) = zero tauctyl(i) = zero do_gwc(i) = .false. @@ -954,7 +976,7 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & ! 1 - nonlin*|c2|. ! !----------------------------------------------------------------------- -!> -# Calculate the minimum Richardson number including both the +!> - Calculate the minimum Richardson number including both the !! basic-state condition and wave effects. !!\f[ !! Ri_{min}\approx\frac{Ri(1-\mu|c_{2}|)}{(1+\mu Ri^{1/2}|c_{2}|)^{2}} @@ -1009,7 +1031,7 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & !----------------------------------------------------------------------- ! -!> -# Calculate the gravity wave stress profile using the wave +!> - Calculate the gravity wave stress profile using the wave !! saturation hypothesis of Lindzen (1981) \cite lindzen_1981. ! ! Assuming kcldtop(i)=10 and kcldbot=16, @@ -1155,7 +1177,7 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & !!!!!! Vertical differentiation !!!!!! -!> -# Calculate wind tendency in direction to the wind vector,zonal +!> - Calculate wind tendency in direction to the wind vector,zonal !! wind tendency and meridional wind tendency above the cloud top !! level due to convectively generated gravity waves. @@ -1373,7 +1395,7 @@ subroutine gwdc_run (im,ix,iy,km,lat,u1,v1,t1,q1,deltim, & ! enddo !----------------------------------------------------------------------- -!> -# Convert back local convective GWD tendency arrays to GFS model +!> - Convert back local convective GWD tendency arrays to GFS model !! vertical indices. ! Outgoing (FU1,FV1)=(utgwc,vtgwc) !----------------------------------------------------------------------- diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 4574fc8b4..4dbb0e4a6 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -50,8 +50,6 @@ !! trigger condition. Convective cloudiness is enhanced by considering suspended !! cloud condensate in the updraft. The lateral entrainment is also enhanced !! to more strongly suppress convection in a drier environment. -!! -!! \section intraphysics Intraphysics Communication !! diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 48eb13e42..815de6e75 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -1,9 +1,99 @@ !> \file mfshalcnv.f !! This file contains the entire SAMF deep convection scheme. + + module sasas_shal_post + contains + +! \brief Brief description of the subroutine +! +!! \section arg_table_sasasshal_post_run Argument Table +!! | local var name | longname | description | units | rank | type | +!! |----------------|----------------------------------------------------------|----------------------------------------------------------------------|---------|------|-------------------------------|-- +!! | frain | dynamics_to_physics_timestep_ratio | ratio of dynamics timestep to physics timestep | none | 0 | real | k +!! | rain1 | lwe_thickness_of_shallow_convective_precipitation_amount | shallow convective rainfall amount on physics timestep | m | 1 | real | k +!! | cnvc | convective_cloud_cover | convective cloud cover | frac | 2 | real | k +!! | cnvw | convective_cloud_water_specific_humidity | convective cloud water specific humidity | kg kg-1 | 2 | real | k +!! | Model | FV3-GFS_Control_type | Fortran DDT containing FV3-GFS model control parameters | DDT | 0 | GFS_control_type | +!! | Grid | FV3-GFS_Grid_type | Fortran DDT containing FV3-GFS grid and interpolation related data | DDT | 0 | GFS_grid_type | +!! | Diag | FV3-GFS_Diag_type | Fortran DDT containing FV3-GFS fields targeted for diagnostic output | DDT | 0 | GFS_diag_type | +!! | Tbd | FV3-GFS_Tbd_type | Fortran DDT containing FV3-GFS miscellaneous data | DDT | 0 | GFS_tbd_type | +!! + subroutine sasasshal_post_run (frain, rain1, cnvc, cnvw, Model, & + & Grid, Diag, Tbd) + + use machine, only: kind_phys + use GFS_typedefs, only: GFS_control_type, & + & GFS_grid_type, GFS_diag_type, GFS_tbd_type + + type(GFS_grid_type), intent(in) :: Grid + type(GFS_control_type), intent(in) :: Model + type(GFS_diag_type), intent(inout) :: Diag + type(GFS_tbd_type), intent(inout) :: Tbd + + real(kind=kind_phys), intent(in) :: frain + real(kind=kind_phys), dimension(size(Grid%xlon,1)), & + & intent(in) :: rain1 + real(kind=kind_phys), dimension(size(Grid%xlon,1),Model%levs), & + & intent(in) :: cnvw, cnvc + + real(kind=kind_phys), dimension(size(Grid%xlon,1)) :: raincs + integer :: num2, num3 + + raincs(:) = frain * rain1(:) + Diag%rainc(:) = Diag%rainc(:) + raincs(:) + if (Model%lssav) then + Diag%cnvprcp(:) = Diag%cnvprcp(:) + raincs(:) + endif + if ((Model%shcnvcw) .and. (Model%num_p3d == 4) .and. & + & (Model%npdf3d == 3)) then + num2 = Model%num_p3d + 2 + num3 = num2 + 1 + Tbd%phy_f3d(:,:,num2) = cnvw(:,:) + Tbd%phy_f3d(:,:,num3) = cnvc(:,:) + elseif ((Model%npdf3d == 0) .and. (Model%ncnvcld3d == 1)) then + num2 = Model%num_p3d + 1 + Tbd%phy_f3d(:,:,num2) = cnvw(:,:) + endif + + end subroutine sasasshal_post_run + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_post_init Argument Table +! + subroutine sasasshal_post_init () + end subroutine sasasshal_post_init + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_post_finalize Argument Table +! + subroutine sasasshal_post_finalize () + end subroutine sasasshal_post_finalize + + end module sasas_shal_post + + module sasas_shal contains + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_init Argument Table +! + subroutine sasasshal_init + end subroutine sasasshal_init + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasshal_init Argument Table +! + subroutine sasasshal_finalize + end subroutine sasasshal_finalize + + !> \defgroup SAMF_shal GFS Scale-Aware Mass-Flux Shallow Convection !> @{ !! \brief The scale-aware mass-flux shallow (SAMF_shal) convection @@ -19,25 +109,15 @@ module sasas_shal !! the level where \f$p=0.7p_{sfc}\f$. The paramerization of scale and !! aerosol awareness follows that of the SAMF deep convection scheme. !! -!! The previous version of the shallow convection scheme (shalcnv.f) +!! The previous version of the shallow convection scheme (\c shalcnv.f) !! is described in Han and Pan (2011) \cite han_and_pan_2011 and differences -!! between the shallow and deep convection schemes are presented in +!! between the shallow and deep convection schemes are presented in !! Han and Pan (2011) \cite han_and_pan_2011 and Han et al. (2017) !! \cite han_et_al_2017 . Details of scale- and aerosol-aware parameterizations !! are described in Han et al. (2017) \cite han_et_al_2017 . -!! -!! \section intraphysics_deep Intraphysics Communication -!! - -! \brief Brief description of the subroutine -! -! \section arg_table_sasasshal_init Argument Table -! - subroutine sasasshal_init - end subroutine sasasshal_init - !>\defgroup SAMF_shal_main GFS mfshalcnv Main !!\ingroup SAMF_shal +!! @{ !> \brief The subroutine contains the entirety of the SAMF shallow convection scheme. !! !! This routine follows the \ref SAMF deep scheme quite closely, although @@ -1704,85 +1784,8 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & return !! @} end subroutine sasasshal_run - -! \brief Brief description of the subroutine -! -!> \section arg_table_sasasshal_init Argument Table -!! - subroutine sasasshal_finalize - end subroutine sasasshal_finalize - +!! @} !> @} - end module sasas_shal - - module sasas_shal_post - contains - -! \brief Brief description of the subroutine -! -!! \section arg_table_sasasshal_post_run Argument Table -!! | local var name | longname | description | units | rank | type | kind | intent | optional | -!! |----------------|----------------------------------------------------------|----------------------------------------------------------------------|---------|------|-------------------------------|-----------|--------|----------| -!! | frain | dynamics_to_physics_timestep_ratio | ratio of dynamics timestep to physics timestep | none | 0 | real | kind_phys | in | F | -!! | rain1 | lwe_thickness_of_shallow_convective_precipitation_amount | shallow convective rainfall amount on physics timestep | m | 1 | real | kind_phys | in | F | -!! | cnvc | convective_cloud_cover | convective cloud cover | frac | 2 | real | kind_phys | in | F | -!! | cnvw | convective_cloud_water_specific_humidity | convective cloud water specific humidity | kg kg-1 | 2 | real | kind_phys | in | F | -!! | Model | FV3-GFS_Control_type | Fortran DDT containing FV3-GFS model control parameters | DDT | 0 | GFS_control_type | | in | F | -!! | Grid | FV3-GFS_Grid_type | Fortran DDT containing FV3-GFS grid and interpolation related data | DDT | 0 | GFS_grid_type | | in | F | -!! | Diag | FV3-GFS_Diag_type | Fortran DDT containing FV3-GFS fields targeted for diagnostic output | DDT | 0 | GFS_diag_type | | inout | F | -!! | Tbd | FV3-GFS_Tbd_type | Fortran DDT containing FV3-GFS miscellaneous data | DDT | 0 | GFS_tbd_type | | inout | F | -!! - subroutine sasasshal_post_run (frain, rain1, cnvc, cnvw, Model, & - & Grid, Diag, Tbd) - - use machine, only: kind_phys - use GFS_typedefs, only: GFS_control_type, & - & GFS_grid_type, GFS_diag_type, GFS_tbd_type - - type(GFS_grid_type), intent(in) :: Grid - type(GFS_control_type), intent(in) :: Model - type(GFS_diag_type), intent(inout) :: Diag - type(GFS_tbd_type), intent(inout) :: Tbd - - real(kind=kind_phys), intent(in) :: frain - real(kind=kind_phys), dimension(size(Grid%xlon,1)), & - & intent(in) :: rain1 - real(kind=kind_phys), dimension(size(Grid%xlon,1),Model%levs), & - & intent(in) :: cnvw, cnvc - - real(kind=kind_phys), dimension(size(Grid%xlon,1)) :: raincs - integer :: num2, num3 - - raincs(:) = frain * rain1(:) - Diag%rainc(:) = Diag%rainc(:) + raincs(:) - if (Model%lssav) then - Diag%cnvprcp(:) = Diag%cnvprcp(:) + raincs(:) - endif - if ((Model%shcnvcw) .and. (Model%num_p3d == 4) .and. & - & (Model%npdf3d == 3)) then - num2 = Model%num_p3d + 2 - num3 = num2 + 1 - Tbd%phy_f3d(:,:,num2) = cnvw(:,:) - Tbd%phy_f3d(:,:,num3) = cnvc(:,:) - elseif ((Model%npdf3d == 0) .and. (Model%ncnvcld3d == 1)) then - num2 = Model%num_p3d + 1 - Tbd%phy_f3d(:,:,num2) = cnvw(:,:) - endif - - end subroutine sasasshal_post_run - -! \brief Brief description of the subroutine -! -! \section arg_table_sasasshal_post_init Argument Table -! - subroutine sasasshal_post_init () - end subroutine sasasshal_post_init -! \brief Brief description of the subroutine -! -! \section arg_table_sasasshal_post_finalize Argument Table -! - subroutine sasasshal_post_finalize () - end subroutine sasasshal_post_finalize + end module sasas_shal - end module sasas_shal_post diff --git a/physics/module_nst_model.f90 b/physics/module_nst_model.f90 index 4f83077fd..a5c31808f 100644 --- a/physics/module_nst_model.f90 +++ b/physics/module_nst_model.f90 @@ -1,5 +1,5 @@ !>\file module_nst_model.f90 -!>\defgroup nst_module Diurnal Thermocline Model +!>\defgroup nst_module GFS NSST Diurnal Thermocline Model !! @{ !>\ingroup GFS_NSST !!\brief This is the module of diurnal thermocline layer model (DTM). @@ -19,6 +19,7 @@ module nst_module contains +!> This subroutine contains the module of diurnal thermocline layer model. subroutine dtm_1p(kdt,timestep,rich,tox,toy,i0,q,sss,sep,q_ts,hl_ts,rho, & alpha,beta,alon,sinlat,soltim,grav,le,d_conv, & xt,xs,xu,xv,xz,xzts,xtts) @@ -78,6 +79,7 @@ subroutine dtm_1p(kdt,timestep,rich,tox,toy,i0,q,sss,sep,q_ts,hl_ts,rho, & end subroutine dtm_1p +!> This subroutine integrates one time step with modified Euler method. subroutine eulerm(kdt,timestep,rich,tox,toy,i0,q,sss,sep,q_ts,hl_ts,rho,alpha,& beta,alon,sinlat,soltim,grav,le,d_conv, & xt,xs,xu,xv,xz,xzts,xtts) @@ -297,6 +299,7 @@ subroutine dtm_1p_zwa(kdt,timestep,i0,q,rho,d_conv,xt,xs,xu,xv,xz,tr_mda,tr_fca, end subroutine dtm_1p_zwa +!> This subroutine applies free convection adjustment(fca). subroutine dtm_1p_fca(d_conv,xt,xtts,xz,xzts) ! apply xz adjustment: free convection adjustment (fca); @@ -313,6 +316,7 @@ subroutine dtm_1p_fca(d_conv,xt,xtts,xz,xzts) end subroutine dtm_1p_fca +!> This subroutine applies top layer adjustment (tla). subroutine dtm_1p_tla(dz,te,xt,xtts,xz,xzts) ! apply xz adjustment: top layer adjustment (tla); @@ -331,6 +335,7 @@ subroutine dtm_1p_tla(dz,te,xt,xtts,xz,xzts) ! xzts = xtts*(1.0+0.5*(2.0*xt-dz*te)/sqrt(xt*(xt-dz*te)))/te end subroutine dtm_1p_tla +!> This subroutine applies maximum warming adjustment (mwa). subroutine dtm_1p_mwa(xt,xtts,xz,xzts) ! apply xz adjustment: maximum warming adjustment (mwa) @@ -343,6 +348,7 @@ subroutine dtm_1p_mwa(xt,xtts,xz,xzts) ! xzts = 2.0*xtts/tw_max end subroutine dtm_1p_mwa +!>This subroutine applies minimum depth adjustment (xz adjustment). subroutine dtm_1p_mda(xt,xtts,xz,xzts) ! apply xz adjustment: minimum depth adjustment (mda) @@ -358,6 +364,7 @@ subroutine dtm_1p_mda(xt,xtts,xz,xzts) end subroutine dtm_1p_mda +!> This subroutine applies maximum temperature adjustment (mta). subroutine dtm_1p_mta(dta,xt,xtts,xz,xzts) ! apply xz adjustment: maximum temperature adjustment (mta) @@ -377,6 +384,7 @@ subroutine dtm_1p_mta(dta,xt,xtts,xz,xzts) end subroutine dtm_1p_mta +!> This subroutine calculates depth for convective adjustment. subroutine convdepth(kdt,timestep,i0,q,sss,sep,rho,alpha,beta,xt,xs,xz,d_conv) ! @@ -613,6 +621,8 @@ subroutine dtm_onset(kdt,timestep,rich,tox,toy,i0,q,sss,sep,q_ts,hl_ts,rho, & end subroutine dtm_onset +!> This subroutine computes coefficients (\a w_0 and \a w_d) to +!! calculate d(tw)/d(ts). subroutine cal_w(kdt,xz,xt,xzts,xtts,w_0,w_d) ! ! abstract: calculate w_0,w_d @@ -642,7 +652,8 @@ subroutine cal_w(kdt,xz,xt,xzts,xtts,w_0,w_d) ! endif end subroutine cal_w - +!> This subroutine calculates the diurnal warming amount at the top layer +!! with thickness of \a delz. subroutine cal_ttop(kdt,timestep,q_warm,rho,dz,xt,xz,ttop) ! ! abstract: calculate @@ -776,6 +787,8 @@ subroutine cal_tztr(kdt,xt,c_0,c_d,w_0,w_d,zc,zw,z,tztr) ! write(*,'(a,i4,9f9.4))') ' cal_tztr : ',kdt,xt,c_0,c_d,w_0,w_d,zc,zw,z,tztr end subroutine cal_tztr +!> This subroutine contains the upper ocean cool-skin parameterization +!! (Fairall et al, 1996 \cite fairall_et_al_1996). subroutine cool_skin(ustar_a,f_nsol,f_sol_0,evap,sss,alpha,beta,rho_w,rho_a,ts,q_ts,hl_ts,grav,le,deltat_c,z_c,c_0,c_d) ! ! upper ocean cool-skin parameterizaion, fairall et al, 1996. diff --git a/physics/module_nst_parameters.f90 b/physics/module_nst_parameters.f90 index 4845c383f..8c8811832 100644 --- a/physics/module_nst_parameters.f90 +++ b/physics/module_nst_parameters.f90 @@ -1,6 +1,8 @@ !>\file module_nst_parameters.f90 -!>\defgroup nst_parameters NST Parameters Module +!>\defgroup nst_parameters GFS NSST Parameter Module !! \ingroup GFS_NSST +!!\brief This module includes constants and parameters used in GFS +!! near sea surface temperature scheme. !! @{ module module_nst_parameters use machine, only : kind_phys & @@ -27,56 +29,45 @@ module module_nst_parameters niter_z_w = 5, & niter_sfs = 5 real (kind=kind_phys), parameter :: & - ! - ! general constants sec_in_day=86400. & ,sec_in_hour=3600. & ,solar_time_6am=21600.0 & - ,const_rot=0.000073 & ! constant to calculate corioli force + ,const_rot=0.000073 & !< constant to calculate corioli force ,ri_c=0.65 & ,ri_g=0.25 & - ,eps_z_w=0.01 & ! criteria to finish iterations for z_w - ,eps_conv=0.01 & ! criteria to finish iterations for d_conv - ,eps_sfs=0.01 & ! criteria to finish iterations for d_sfs - ,z_w_max=30.0 & ! max warm layer thickness -! ,z_w_max=100.0 & ! max warm layer thickness - ,z_w_min=0.2 & ! min warm layer thickness - ,z_w_ini=0.2 & ! initial warm layer thickness in dtl_onset - ,z_c_max=0.01 & ! maximum of sub-layer thickness (m) - ,z_c_ini=0.001 & ! initial value of z_c - ,ustar_a_min=0.031 & ! minimum of friction wind speed (m/s): 0.031 ~ 1m/s at 10 m hight - ,tau_min=0.005 & ! minimum of wind stress for dtm - ,exp_const=9.5 & ! coefficient in exponet profile - ,delz=0.1 & ! vertical increment for integral calculation (m) - ,von=0.4 & ! von karman's "constant" ! - ,t0k=273.16 & ! celsius to kelvin + ,eps_z_w=0.01 & !< criteria to finish iterations for z_w + ,eps_conv=0.01 & !< criteria to finish iterations for d_conv + ,eps_sfs=0.01 & !< criteria to finish iterations for d_sfs + ,z_w_max=30.0 & !< max warm layer thickness + ,z_w_min=0.2 & !< min warm layer thickness + ,z_w_ini=0.2 & !< initial warm layer thickness in dtl_onset + ,z_c_max=0.01 & !< maximum of sub-layer thickness (m) + ,z_c_ini=0.001 & !< initial value of z_c + ,ustar_a_min=0.031 & !< minimum of friction wind speed (m/s): 0.031 ~ 1m/s at 10 m hight + ,tau_min=0.005 & !< minimum of wind stress for dtm + ,exp_const=9.5 & !< coefficient in exponet profile + ,delz=0.1 & !< vertical increment for integral calculation (m) + ,von=0.4 & !< von karman's "constant" + ,t0k=273.16 & !< celsius to kelvin ,gray=0.97 & ,sst_max=308.16 & ,tw_max=5.0 & ,wd_max=2.0 & - ,omg_m =1.0 & ! trace factor to apply salinity effect - ,omg_rot = 1.0 & ! trace factor to apply rotation effect - ,omg_sh = 1.0 & ! trace factor to apply sensible heat due to rainfall effect -!dbgz - ,visw=1.e-6 & !m2/s kinematic viscosity water + ,omg_m =1.0 & !< trace factor to apply salinity effect + ,omg_rot = 1.0 & !< trace factor to apply rotation effect + ,omg_sh = 1.0 & !< trace factor to apply sensible heat due to rainfall effect + ,visw=1.e-6 & !< m2/s kinematic viscosity water ,novalue=0 & -! ,novalue=-1.0e+10 & ,smallnumber=1.e-6 & -! ,timestep_oc=sec_in_day/24. & ! time step in the ocean model (1 hours) - ,timestep_oc=sec_in_day/8. & ! time step in the ocean model (3 hours) + ,timestep_oc=sec_in_day/8. & !< time step in the ocean model (3 hours) ,radian=2.*pi/180. & ,rad2deg=180./pi & - ! sea constants and coefficients - ! - ,cp_w=4000. & ! specific heat water (j/kg/k ) - ,rho0_w=1022.0 & ! density water (kg/m3 ) (or 1024.438) - ,vis_w=1.e-6 & ! kinematic viscosity water (m2/s ) - ,tc_w=0.6 & ! thermal conductivity water (w/m/k ) - ,capa_w =3950.0 & ! heat capacity of sea water ! - ! - ! air constants and coefficients - ! - ,thref =1.0e-3 ! reference value of specific volume (m**3/kg) + ,cp_w=4000. & !< specific heat water (j/kg/k ) + ,rho0_w=1022.0 & !< density water (kg/m3 ) (or 1024.438) + ,vis_w=1.e-6 & !< kinematic viscosity water (m2/s ) + ,tc_w=0.6 & !< thermal conductivity water (w/m/k ) + ,capa_w =3950.0 & !< heat capacity of sea water ! + ,thref =1.0e-3 !< reference value of specific volume (m**3/kg) !!$!============================================ !!$ diff --git a/physics/module_nst_water_prop.f90 b/physics/module_nst_water_prop.f90 index 2f4d5df6d..b8f4399d1 100644 --- a/physics/module_nst_water_prop.f90 +++ b/physics/module_nst_water_prop.f90 @@ -1,5 +1,5 @@ !>\file module_nst_water_prop.f90 -!>\defgroup nst_water_prop NST Water Prop Module +!>\defgroup nst_water_prop GFS NSST Water Prop Module !! @{ !>\ingroup GFS_NSST !!\brief diff --git a/physics/ozphys.f b/physics/ozphys.f index 1c07e04f7..ce431711b 100644 --- a/physics/ozphys.f +++ b/physics/ozphys.f @@ -1,16 +1,7 @@ !> \file ozphys.f !! This file is ozone sources and sinks. -!> \defgroup GFS_ozn GFS Ozone Sources and Sinks -!! \brief The operational GFS currently parameterizes ozone production and -!! destruction based on monthly mean coefficients provided by Naval -!! Research Laboratory through CHEM2D chemistry model -!! (McCormack et al. 2006 \cite mccormack_et_al_2006). -!! Monthly and zonal mean ozone production rate and ozone destruction -!! rate per unit ozone mixing ratio were provided by NRL based on -!! CHEM2D model. -!! Original version of these terms were provided by NASA/DAO based on -!! NASA 2D Chemistry model - GSM is capable of running both versions +!> \defgroup GFS_ozn GFS Ozone Physics !! !! \section intra_oz Intraphysics Communication !! @@ -51,7 +42,10 @@ end subroutine ozphys_init !>\defgroup GFS_ozphys GFS ozphys Main !>\ingroup GFS_ozn -!! \brief This is the main subroutine +!! \brief The operational GFS currently parameterizes ozone production and +!! destruction based on monthly mean coefficients (\c global_o3prdlos.f77) provided by Naval +!! Research Laboratory through CHEM2D chemistry model +!! (McCormack et al. 2006 \cite mccormack_et_al_2006). !! \section arg_table_ozphys_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|---------------------------------------------------|---------------------------------------------------|---------|------|---------|-----------|--------|----------| @@ -99,6 +93,7 @@ subroutine ozphys_run ( & real(kind=kind_phys) wk1(im), wk2(im), wk3(im), prod(im,pl_coeff), & ozib(im), colo3(im,levs+1) ! +!> - Calculate vertical integrated column ozone values. if (pl_coeff > 2) then colo3(:,levs+1) = 0.0 do l=levs,1,-1 @@ -108,6 +103,7 @@ subroutine ozphys_run ( & enddo endif ! +!> - Apply vertically linear interpolation to the ozone coefficients. do l=1,levs pmin = 1.0e10 pmax = -1.0e10 @@ -169,7 +165,11 @@ subroutine ozphys_run ( & enddo endif endif - +!> - Calculate the 4 terms of prognostic ozone change during time \a dt: +!! - ozp(:,:,1) - Ozone production at model layers +!! - ozp(:,:,2) - Ozone tendency at model layers +!! - ozp(:,:,3) - Ozone production from temperature term at model layers +!! - ozp(:,:,4) - Ozone production from column ozone term at model layers if (pl_coeff == 4) then do i=1,im ozib(i) = ozi(i,l) ! no filling diff --git a/physics/radlw_main.f b/physics/radlw_main.f index 05dbdc071..ade840b94 100644 --- a/physics/radlw_main.f +++ b/physics/radlw_main.f @@ -2,7 +2,7 @@ !! This file contains NCEP's modifications of the rrtmg-lw radiation !! code from AER. -!>\defgroup RRTMG GFS RRTMG Shortwave/Longwave Radiation Scheme +!>\defgroup RRTMG GFS RRTMG Shortwave/Longwave Radiation !! \brief The GFS radiation scheme !! \details Radiative processes are among the most complex and !! computationally intensive parts of all model physics. As an diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index 6aa708f0d..0376357e5 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -12,7 +12,7 @@ end subroutine sfc_ex_coef_init subroutine sfc_ex_coef_finalize end subroutine sfc_ex_coef_finalize -!> \defgroup Sfc_ex_cal GFS Surface Sublayer Scheme +!> \defgroup Sfc_ex_cal GFS Surface Layer !! !> \defgroup GFS_diff_main GFS sfc_diff Main !! \ingroup Sfc_ex_cal diff --git a/physics/sfc_drv.f b/physics/sfc_drv.f index 043ea4437..09619d3d4 100644 --- a/physics/sfc_drv.f +++ b/physics/sfc_drv.f @@ -1,66 +1,7 @@ !> \file sfc_drv.f !! This file contains the Noah land surface scheme driver. -!> \defgroup NOAH GFS Noah Land Surface Scheme -!! \brief This it the Noah Land Surface Model (Noah LSM). -!! -!! Land-atmosphere interactions are a main driver of Earth's surface -!! water and energy budgets. The importance of the land surface is -!! rather intuitive, and has been demonstrated not only in terms of -!! predictability on daily to seasonal timescale (Betts et al. 2017 -!! \cite betts_et_al_2017), but also in terms -!! of influencing extremes such as drought and heatwaves (PaiMazumder and -!! Done, 2016 \cite paimazumder_and_done_2016), PBL evolution and cloud -!! formation (Milovac et al. 2016 \cite milovac_et_al_2016) and afternoon -!! convection (Guillod et al. 2015 \cite guillod_et_al_2015), and -!! tropical cyclone re-intensification (Andersen and Shepherd, 2014 -!! \cite andersen_and_shepherd_2014). Other linkages, such as the role of soil -!! moisture (SM) or vegetation heterogeneity in mesoscale circulation -!! (Hsu et al. 2017 \cite hsu_et_al_2017) and planetary waves (Koster -!! et al. 2014 \cite koster_et_al_2014), and those driven by land use -!! and land cover change or management (Hirsch et al. 2015 -!! \cite hirsch_et_al_2015, Findell et al. 2017 -!! \cite findell_et_al_2017) are topics of active research. -!! -!! Figure 1 is a schematic of local land-atmosphere interactions in a -!! quiescent synoptic regime, including the soil moisture-precipitation -!! (SM-P) feedback pathways. Solid arrows indicate a positive feedback -!! pathway, and large dashed arrows represent a negative feedback, while -!! red indicates radiative, black indicates surface layer and PBL, and -!! brown indicates land surface processes. Thin red and grey dashed lines -!! with arrows also represent positive feedbacks. The single horizontal -!! gay-dotted line (no arrows) indicates the top of the PBL, and the seven -!! small vertical dashed lines (no arrows) represent precipitation -!! \image html Noah_LA_interaction.png "Figure 1: Local Land-atmosphere Interaction (courtesy of Micheal Ek, Ek and Mahrt (1994), Ek and Holtslag (2004))" width=10cm -!! The land-surface model component was substantially upgraded from the Oregon -!! State University (OSU) land surface model to EMC's new Noah Land Surface Model -!! (Noah LSM) during the major implementation in the NCEP Global Forecast System -!! (GFS) on May 31, 2005. Forecast System (GFS). The Noah LSM embodies about 10 -!! years of upgrades (see Chen et al. 1996 -!! \cite chen_et_al_1996; Koren et al. 1999 \cite koren_et_al_1999; Ek et al. 2003 -!! \cite ek_et_al_2003) to its ancestor, the OSU LSM. The Noah LSM upgrade includes: -!! - An increase from two (10, 190 cm thick) to four soil layers (10, -!! 30, 60, 100 cm thick) -!! - Addition of frozen soil physics -!! - Add glacial ice treatment -!! - Two snowpack states (SWE, density) -!! - New formulations for infiltration and runoff account for sub-grid -!! variability in precipitation and soil moisture -!! - Revised physics of the snowpack and its influence on surface heat -!! fluxes and albedo -!! - Higher canopy resistance -!! - Spatially varying root depth -!! - Surface fluxes weighted by snow cover fraction -!! - Improved thermal conduction in soil/snow -!! - Improved seasonality of green vegetation cover. -!! - Improved evaporation treatment over bare soil and snowpack -!! -!! \image html land_dataset.png "Figure 2: Land Data Sets Used in NCEP Modeling Systems" width=10cm -!! -!!\section Intraphysics Intraphysics Communication -!! ! \defgroup NOAH_pre Noah Land Surface Pre -! \ingroup NOAH ! \brief Brief description of the parameterization ! @{ @@ -125,7 +66,6 @@ end module lsm_noah_pre ! @} ! \defgroup NOAH_post NOAH Land Surface post -! \ingroup NOAH ! @{ ! \brief Brief description of the parameterization ! \section intraphysics Intraphysics Communication @@ -301,12 +241,14 @@ end subroutine lsm_noah_finalize !----------------------------------- ! subroutine sfc_drv & -!> \defgroup NOAH_drv GFS sfc_drv Main -!! \ingroup NOAH -!! @{ -!! \brief This is Noah LSM driver scheme. -!! -!! \section arg_table_lsm_noah_run Argument Table +!> \defgroup Noah_Main GFS Noah Land Surface Model +!> \defgroup Noah_drv GFS Noah LSM Driver +!!\ingroup Noah_Main +!! \brief This is Noah LSM driver module, with the functionality of +!! preparing variables to run Noah LSM gfssflx(), calling Noah LSM and post-processing +!! variables for return to the parent model suite including unit conversion, as well +!! as diagnotics calculation. +!! \section arg_table_lsm_Noah_run Argument Table !!| local var name | longname | description | units | rank | type | kind | intent | optional | !!|----------------|------------------------------------------------------------------------------|-----------------------------------------------------------------|------------|------|---------|-----------|--------|----------| !!| im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | @@ -373,9 +315,10 @@ end subroutine lsm_noah_finalize !!| smcref2 | threshold_volume_fraction_of_condensed_water_in_soil | soil moisture threshold | frac | 1 | real | kind_phys | out | F | !!| wet1 | normalized_soil_wetness | normalized soil wetness | frac | 1 | real | kind_phys | out | F | !! -!! \section general_noah General Algorithm -!! \section detailed_noah Detailed Algorithm +!! \section general_noah_drv General Algorithm !! @{ +! \section detailed_noah Detailed Algorithm +! @{ subroutine lsm_noah_run & & ( im, km, ps, u1, v1, t1, q1, soiltyp, vegtype, sigmaf, & & sfcemis, dlwflx, dswsfc, snet, delt, tg3, cm, ch, & @@ -470,13 +413,13 @@ subroutine lsm_noah_run & !===> ... begin here ! -! --- ... set flag for land points +!> - Set flag for land points. do i = 1, im flag(i) = (islimsk(i) == 1) enddo -! --- ... save land-related prognostic fields for guess run +!> - Save land-related prognostic fields for guess run. do i = 1, im if (flag(i) .and. flag_guess(i)) then @@ -543,16 +486,16 @@ subroutine lsm_noah_run & do i = 1, im if (flag_iter(i) .and. flag(i)) then -! --- ... noah: prepare variables to run noah lsm -! 1. configuration information (c): -! ------------------------------ -! couple - couple-uncouple flag (=1: coupled, =0: uncoupled) -! ffrozp - flag for snow-rain detection (1.=snow, 0.=rain) -! ice - sea-ice flag (=1: sea-ice, =0: land) -! dt - timestep (sec) (dt should not exceed 3600 secs) = delt -! zlvl - height (m) above ground of atmospheric forcing variables -! nsoil - number of soil layers (at least 2) -! sldpth - the thickness of each soil layer (m) +!> - Prepare variables to run Noah LSM: +!! - 1. configuration information (c): +!!\n ---------------------------------------- +!!\n \a couple - couple-uncouple flag (=1: coupled, =0: uncoupled) +!!\n \a ffrozp - flag for snow-rain detection (1.=snow, 0.=rain) +!!\n \a ice - sea-ice flag (=1: sea-ice, =0: land) +!!\n \a dt - timestep (sec) (dt should not exceed 3600 secs) = delt +!!\n \a zlvl - height (\f$m\f$) above ground of atmospheric forcing variables +!!\n \a nsoil - number of soil layers (at least 2) +!!\n \a sldpth - the thickness of each soil layer (\f$m\f$) couple = 1 ! run noah lsm in 'couple' mode @@ -571,15 +514,15 @@ subroutine lsm_noah_run & sldpth(k) = zsoil(i,k-1) - zsoil(i,k) enddo -! 2. forcing data (f): -! ----------------- -! lwdn - lw dw radiation flux (w/m2) -! solnet - net sw radiation flux (dn-up) (w/m2) -! sfcprs - pressure at height zlvl above ground (pascals) -! prcp - precip rate (kg m-2 s-1) -! sfctmp - air temperature (k) at height zlvl above ground -! th2 - air potential temperature (k) at height zlvl above ground -! q2 - mixing ratio at height zlvl above ground (kg kg-1) +!> - 2. forcing data (f): +!!\n --------------------------------------- +!!\n \a lwdn - lw dw radiation flux (\f$W m^{-2}\f$) +!!\n \a solnet - net sw radiation flux (dn-up) (\f$W m^{-2}\f$) +!!\n \a sfcprs - pressure at height zlvl above ground (pascals) +!!\n \a prcp - precip rate (\f$kg m^{-2} s^{-1}\f$) +!!\n \a sfctmp - air temperature (\f$K\f$) at height zlvl above ground +!!\n \a th2 - air potential temperature (\f$K\f$) at height zlvl above ground +!!\n \a q2 - mixing ratio at height zlvl above ground (\f$kg kg^{-1}\f$) lwdn = dlwflx(i) !..downward lw flux at sfc in w/m2 swdn = dswsfc(i) !..downward sw flux at sfc in w/m2 @@ -592,27 +535,27 @@ subroutine lsm_noah_run & th2 = theta1(i) q2 = q0(i) -! 3. other forcing (input) data (i): -! ------------------------------ -! sfcspd - wind speed (m s-1) at height zlvl above ground -! q2sat - sat mixing ratio at height zlvl above ground (kg kg-1) -! dqsdt2 - slope of sat specific humidity curve at t=sfctmp (kg kg-1 k-1) +!> - 3. other forcing (input) data (i): +!!\n --------------------------------------- +!!\n \a sfcspd - wind speed (\f$m s^{-1}\f$) at height zlvl above ground +!!\n \a q2sat - sat mixing ratio at height zlvl above ground (\f$kg kg^{-1}\f$) +!!\n \a dqsdt2 - slope of sat specific humidity curve at t=sfctmp (\f$kg kg^{-1} k^{-1}\f$) sfcspd = wind(i) q2sat = qs1(i) dqsdt2 = q2sat * a23m4/(sfctmp-a4)**2 -! 4. canopy/soil characteristics (s): -! -------------------------------- -! vegtyp - vegetation type (integer index) -> vtype -! soiltyp - soil type (integer index) -> stype -! slopetyp- class of sfc slope (integer index) -> slope -! shdfac - areal fractional coverage of green vegetation (0.0-1.0) -! shdmin - minimum areal fractional coverage of green vegetation -> shdmin1d -! ptu - photo thermal unit (plant phenology for annuals/crops) -! alb - backround snow-free surface albedo (fraction) -! snoalb - upper bound on maximum albedo over deep snow -> snoalb1d -! tbot - bottom soil temperature (local yearly-mean sfc air temp) +!> - 4. canopy/soil characteristics (s): +!!\n ------------------------------------ +!!\n \a vegtyp - vegetation type (integer index) -> vtype +!!\n \a soiltyp - soil type (integer index) -> stype +!!\n \a slopetyp- class of sfc slope (integer index) -> slope +!!\n \a shdfac - areal fractional coverage of green vegetation (0.0-1.0) +!!\n \a shdmin - minimum areal fractional coverage of green vegetation -> shdmin1d +!!\n \a ptu - photo thermal unit (plant phenology for annuals/crops) +!!\n \a alb - backround snow-free surface albedo (fraction) +!!\n \a snoalb - upper bound on maximum albedo over deep snow -> snoalb1d +!!\n \a tbot - bottom soil temperature (local yearly-mean sfc air temp) vtype = vegtype(i) stype = soiltyp(i) @@ -627,18 +570,19 @@ subroutine lsm_noah_run & alb = sfalb(i) tbot = tg3(i) -! 5. history (state) variables (h): -! ------------------------------ -! cmc - canopy moisture content (m) -! t1 - ground/canopy/snowpack) effective skin temperature (k) -> tsea -! stc(nsoil) - soil temp (k) -> stsoil -! smc(nsoil) - total soil moisture content (volumetric fraction) -> smsoil -! sh2o(nsoil)- unfrozen soil moisture content (volumetric fraction) -> slsoil -! snowh - actual snow depth (m) -! sneqv - liquid water-equivalent snow depth (m) -! albedo - surface albedo including snow effect (unitless fraction) -! ch - surface exchange coefficient for heat and moisture (m s-1) -> chx -! cm - surface exchange coefficient for momentum (m s-1) -> cmx +!> - 5. history (state) variables (h): +!!\n ------------------------------ +!!\n \a cmc - canopy moisture content (\f$m\f$) +!!\n \a t1 - ground/canopy/snowpack effective skin temperature (\f$K\f$) -> tsea +!!\n \a stc(nsoil) - soil temp (\f$K\f$) -> stsoil +!!\n \a smc(nsoil) - total soil moisture content (volumetric fraction) -> smsoil +!!\n \a sh2o(nsoil)- unfrozen soil moisture content (volumetric fraction) -> slsoil +!!\n \a snowh - actual snow depth (\f$m\f$) +!!\n \a sneqv - liquid water-equivalent snow depth (\f$m\f$) +!!\n \a albedo - surface albedo including snow effect (unitless fraction) +!!\n \a ch - surface exchange coefficient for heat and moisture (\f$m s^{-1}\f$) -> chx +!!\n \a cm - surface exchange coefficient for momentum (\f$m s^{-1}\f$) -> cmx +!!\n \a z0 - surface roughness (\f$m\f$) -> zorl(\f$cm\f$) cmc = canopy(i) * 0.001 ! convert from mm to m tsea = tsurf(i) ! clu_q2m_iter @@ -663,9 +607,10 @@ subroutine lsm_noah_run & ! ---- ... outside sflx, roughness uses cm as unit z0 = zorl(i)/100. -! --- ... call noah lsm +!> - Call Noah LSM gfssflx(). - call sflx & +! call sflx & + call gfssflx & ! ccppdox: these is sflx in mpbl ! --- inputs: & ( nsoil, couple, ice, ffrozp, delt, zlvl, sldpth, & & swdn, solnet, lwdn, sfcems, sfcprs, sfctmp, & @@ -681,16 +626,16 @@ subroutine lsm_noah_run & & snomlt, sncovr, rc, pc, rsmin, xlai, rcs, rct, rcq, & & rcsoil, soilw, soilm, smcwlt, smcdry, smcref, smcmax) -! --- ... noah: prepare variables for return to parent mode -! 6. output (o): -! ----------- -! eta - actual latent heat flux (w m-2: positive, if upward from sfc) -! sheat - sensible heat flux (w m-2: positive, if upward from sfc) -! beta - ratio of actual/potential evap (dimensionless) -! etp - potential evaporation (w m-2) -! ssoil - soil heat flux (w m-2: negative if downward from surface) -! runoff1 - surface runoff (m s-1), not infiltrating the surface -! runoff2 - subsurface runoff (m s-1), drainage out bottom +!> - Noah LSM: prepare variables for return to parent model and unit conversion. +!> - 6. output (o): +!!\n ------------------------------ +!!\n \a eta - actual latent heat flux (\f$W m^{-2}\f$: positive, if upward from sfc) +!!\n \a sheat - sensible heat flux (\f$W m^{-2}\f$: positive, if upward from sfc) +!!\n \a beta - ratio of actual/potential evap (dimensionless) +!!\n \a etp - potential evaporation (\f$W m^{-2}\f$) +!!\n \a ssoil - soil heat flux (\f$W m^{-2}\f$: negative if downward from surface) +!!\n \a runoff1 - surface runoff (\f$m s^{-1}\f$), not infiltrating the surface +!!\n \a runoff2 - subsurface runoff (\f$m s^{-1}\f$), drainage out bottom evap(i) = eta hflx(i) = sheat @@ -772,7 +717,7 @@ subroutine lsm_noah_run & endif ! end if_flag_iter_and_flag_block enddo ! end do_i_loop -! --- ... compute qsurf (specific humidity at sfc) +!> - Compute specific humidity at surface (\a qsurf). do i = 1, im if (flag_iter(i) .and. flag(i)) then @@ -781,6 +726,8 @@ subroutine lsm_noah_run & endif enddo +!> - Compute surface upward sensible heat flux (\a hflx) and evaporation +!! flux (\a evap). do i = 1, im if (flag_iter(i) .and. flag(i)) then tem = 1.0 / rho(i) @@ -789,7 +736,7 @@ subroutine lsm_noah_run & endif enddo -! --- ... restore land-related prognostic fields for guess run +!> - Restore land-related prognostic fields for guess run. do i = 1, im if (flag(i)) then @@ -817,7 +764,6 @@ subroutine lsm_noah_run & ! end subroutine sfc_drv end subroutine lsm_noah_run !----------------------------------- -!! @} !! @} end module lsm_noah diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index 5a9e7a96b..84100fca5 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -20,11 +20,10 @@ end subroutine sfc_nst_init subroutine sfc_nst_finalize end subroutine sfc_nst_finalize -!> \defgroup GFS_NSST GFS Near Sea Surface Temperature -!>\defgroup gfs_nst_main GFS sfc_nst Main +!> \defgroup GFS_NSST GFS Near Sea Surface Temperature +!>\defgroup gfs_nst_main GFS NSST Main !!\ingroup GFS_NSST -!> \brief This is the second subroutine called in surface land loop. -!!This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. +!> \brief This subroutine calls the Thermal Skin-layer and Diurnal Thermocline models to update the NSST profile. !! \section arg_table_sfc_nst_run Argument Table !! | local var name | longname | description | units | rank | type | kind | intent | optional | !! |----------------|------------------------------------------------------------------------------|-------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| @@ -88,13 +87,11 @@ end subroutine sfc_nst_finalize !! | ep | surface_upward_potential_latent_heat_flux | potential evaporation | W m-2 | 1 | real | kind_phys | out | F | !! !! \section NSST_general_algorithm General Algorithm -!! -!! This is the main subroutine for the NSST scheme, and it calls the DTM and TSM. -!! -!! \section NSST_detailed_algorithm Detailed Algorithm -!! -!! !> @{ +! \section NSST_detailed_algorithm Detailed Algorithm +! +! +! @{ subroutine sfc_nst_run & & ( im, km, ps, u1, v1, t1, q1, tref, cm, ch, & & prsl1, prslki, islimsk, xlon, sinlat, stress, & @@ -373,7 +370,7 @@ subroutine sfc_nst_run & cmm(i) = cm (i) * wind(i) chh(i) = rho_a(i) * ch(i) * wind(i) -! --- ... latent and sensible heat flux over open water with tskin +!> - Calculate latent and sensible heat flux over open water with tskin. ! at previous time step evap(i) = elocp * rch(i) * (qss(i) - q0(i)) qsurf(i) = qss(i) @@ -390,6 +387,9 @@ subroutine sfc_nst_run & zsea1 = 0.001*real(nstf_name4) zsea2 = 0.001*real(nstf_name5) +!> - Call module_nst_water_prop::density() to compute sea water density. +!> - Call module_nst_water_prop::rhocoef() to compute thermal expansion +!! coefficient (\a alpha) and saline contraction coefficient (\a beta). do i = 1, im if ( flag(i) ) then tsea = tsurf(i) @@ -401,7 +401,7 @@ subroutine sfc_nst_run & call density(tsea,sss,rho_w) ! sea water density call rhocoef(tsea,sss,rho_w,alpha,beta) ! alpha & beta ! -! calculate sensible heat flux due to rainfall +!> - Calculate sensible heat flux (\a qrain) due to rainfall. ! le = (2.501-.00237*tsea)*1e6 dwat = 2.11e-5*(t1(i)/t0k)**1.94 ! water vapor diffusivity @@ -432,7 +432,9 @@ subroutine sfc_nst_run & rf_ts = (1000.*rain(i)/rho_w)*alfac*cp_w*(1.0+rch(i)*hl_ts) q_ts = rnl_ts + hs_ts + hl_ts + omg_sh*rf_ts ! -! run sub-layer cooling model/parameterization & calculate c_0, c_d +!> - Call cool_skin(), which is the sub-layer cooling parameterization +!! (Fairall et al, 1996 \cite fairall_et_al_1996). +! & calculate c_0, c_d ! call cool_skin(ustar_a,f_nsol,nswsfc(i),evap(i),sss,alpha,beta &, rho_w,rho_a(i),tsea,q_ts,hl_ts,grav,le @@ -445,7 +447,7 @@ subroutine sfc_nst_run & tauy = max(stress(i),tau_min)*sina fc = const_rot*sinlat(i) ! -! run dtm-1p system +! Run DTM-1p system. ! if ( (soltim > solar_time_6am .and. ifd(i) == 0.0) ) then else @@ -455,6 +457,7 @@ subroutine sfc_nst_run & ! ! if (lprnt .and. i == ipr) print *,' beg xz=',xz(i) +!> - Call convdepth() to calculate depth for convective adjustments. if ( f_nsol > 0.0 .and. xt(i) > 0.0 ) then call convdepth(kdt,timestep,nswsfc(i),f_nsol,sss,sep,rho_w &, alpha,beta,xt(i),xs(i),xz(i),d_conv(i)) @@ -478,6 +481,7 @@ subroutine sfc_nst_run & rich = ri_c +!> - Call the diurnal thermocline layer model dtm_1p(). call dtm_1p(kdt,timestep,rich,taux,tauy,nswsfc(i), & f_nsol,sss,sep,q_ts,hl_ts,rho_w,alpha,beta,alon, & sinlat(i),soltim,grav,le,d_conv(i), @@ -487,8 +491,12 @@ subroutine sfc_nst_run & ! apply mda if ( xt(i) > 0.0 ) then +!> - If \a dtl heat content \a xt > 0.0, call dtm_1p_mda() to apply +!! minimum depth adjustment (mda). call dtm_1p_mda(xt(i),xtts(i),xz(i),xzts(i)) if ( xz(i) >= z_w_max ) then +!> - If \a dtl thickness >= module_nst_parameters::z_w_max, call dtl_reset() +!! to reset xt/xs/x/xv to zero, and xz to module_nst_parameters::z_w_max. call dtl_reset(xt(i),xs(i),xu(i),xv(i),xz(i),xtts(i), & xzts(i)) @@ -498,6 +506,10 @@ subroutine sfc_nst_run & ! apply fca if ( d_conv(i) > 0.0 ) then +!> - If thickness of free convection layer > 0.0, call dtm_1p_fca() +!! to apply free convection adjustment. +!> - If \a dtl thickness >= module_nst_parameters::z_w_max(), call dtl_reset() +!! to reset xt/xs/x/xv to zero, and xz to module_nst_parameters::z_w_max(). call dtm_1p_fca(d_conv(i),xt(i),xtts(i),xz(i),xzts(i)) if ( xz(i) >= z_w_max ) then call dtl_reset @@ -510,8 +522,14 @@ subroutine sfc_nst_run & ! apply tla dz = min(xz(i),max(d_conv(i),delz)) ! +!> - Call sw_ps_9b() to compute the fraction of the solar radiation +!! absorbed by the depth \a delz Paulson and Simpson (1981) \cite paulson_and_simpson_1981. +!! And calculate the total heat absorbed in warm layer. call sw_ps_9b(delz,fw) q_warm = fw*nswsfc(i)-f_nsol !total heat absorbed in warm layer + +!> - Call cal_ttop() to calculate the diurnal warming amount at the top layer with +!! thickness of \a dz. if ( q_warm > 0.0 ) then call cal_ttop(kdt,timestep,q_warm,rho_w,dz, & xt(i),xz(i),ttop0) @@ -527,6 +545,7 @@ subroutine sfc_nst_run & ! &,' ttop=',ttop,' ttop0=',ttop0,' xt=',xt(i),' dz=',dz ! &,' xznew=',(xt(i)+sqrt(xt(i)*(xt(i)-dz*ttop0)))/ttop0 +!> - Call dtm_1p_tla() to apply top layer adjustment. if ( ttop > ttop0 ) then call dtm_1p_tla(dz,ttop0,xt(i),xtts(i),xz(i),xzts(i)) @@ -542,6 +561,7 @@ subroutine sfc_nst_run & ! if (lprnt .and. i == ipr) print *,' beg xz5=',xz(i) ! apply mwa +!> - Call dt_1p_mwa() to apply maximum warming adjustment. t0 = (xt(i)+xt(i))/xz(i) if ( t0 > tw_max ) then call dtm_1p_mwa(xt(i),xtts(i),xz(i),xzts(i)) @@ -554,6 +574,7 @@ subroutine sfc_nst_run & ! if (lprnt .and. i == ipr) print *,' beg xz6=',xz(i) ! apply mta +!> - Call dtm_1p_mta() to apply maximum temperature adjustment. sstc = tref(i) + (xt(i)+xt(i))/xz(i) - dt_cool(i) if ( sstc > sst_max ) then @@ -579,6 +600,7 @@ subroutine sfc_nst_run & ! if (lprnt .and. i == ipr) print *,' beg xz7=',xz(i) ! update tsurf (when flag(i) .eqv. .true. ) +!> - Call get_dtzm_point() to computes \a dtz and \a tsurf. call get_dtzm_point(xt(i),xz(i),dt_cool(i),z_c(i), & zsea1,zsea2,dtz) tsurf(i) = max(271.2, tref(i) + dtz ) @@ -586,6 +608,7 @@ subroutine sfc_nst_run & if (lprnt .and. i == ipr) print *,' tsurf=',tsurf(i),' tref=', &tref(i),' xz=',xz(i),' dt_cool=',dt_cool(i) +!> - Call cal_w() to calculate \a w_0 and \a w_d. if ( xt(i) > 0.0 ) then call cal_w(kdt,xz(i),xt(i),xzts(i),xtts(i),w_0(i),w_d(i)) else @@ -637,8 +660,8 @@ subroutine sfc_nst_run & ! if (lprnt .and. i == ipr) print *,' beg xz8=',xz(i) if ( nstf_name1 > 1 ) then -! --- ... latent and sensible heat flux over open water with updated tskin -! for the grids of open water and the iteration is on +!> - Calculate latent and sensible heat flux over open water with updated tskin +!! for the grids of open water and the iteration is on. do i = 1, im if ( flag(i) ) then qss(i) = fpvs( tskin(i) ) @@ -673,12 +696,9 @@ module sfc_nst_pre contains ! \defgroup GFS_NSST_PRE GFS Near Sea Surface Temperature Pre -!! \brief Brief description of the parameterization -!! -!! Blah blah blah description of parameterization -!! -!! -!! \section intraphysics Intraphysics Communication +! \brief Brief description of the parameterization +! +! \section intraphysics Intraphysics Communication !! !! The NSST scheme is one of the three schemes used to represent the !! surface in the GFS physics suite. The other two are the Noah land diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 5b44b8e06..b12a6a39c 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -1,6 +1,141 @@ !> \file sfc_sice.f !! This file contains the GFS three level thermodynamic sea ice model. + module sfc_sice_pre + contains +! +! \brief This subroutine is empty since there are no procedures needed +! \section arg_table_sfc_sice_pre_init Argument Table +! + subroutine sfc_sice_pre_init + end subroutine sfc_sice_pre_init + +! +! \brief This subroutine is empty since there are no procedures needed +! \section arg_table_sfc_sice_pre_finalize Argument Table +! + subroutine sfc_sice_pre_finalize + end subroutine sfc_sice_pre_finalize + + +! \section arg_table_sfc_sice_pre_run Argument Table +!! | local var name | longname | description | units | rank | type | +!! |----------------|------------------------------------------------------------------------------|-------------------------------------------------------------|---------------|------|---------|---- +!! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | +!! | fice | sea_ice_concentration | sea-ice concentration [0,1] | frac | 1 | real | kin +!! | hice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kin +!! | tisfc | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kin +!! | prsik | exner_function_at_lowest_model_interface | Exner function at lowest model interface | none | 1 | real | kin +!! | prslk | dimensionless_exner_function_at_lowest_model_layer | dimensionless Exner function at lowest model layer | none | 1 | real | kin +!! | cice | sea_ice_concentration | sea-ice concentration [0,1] | frac | 1 | real | kin +!! | zice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kin +!! | tice | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kin +!! | work3 | ratio_of_exner_function_between_midlayer_and_interface_at_lowest_model_layer | Exner function ratio bt midlayer and interface at 1st layer | ratio | 1 | real | kin +!! + subroutine sfc_sice_pre_run(im, fice, hice, tisfc , prsik, prslk, & + & cice, zice, tice, work3) + + use machine, only : kind_phys + + implicit none + +! --- inputs + integer :: im + real(kind=kind_phys), dimension(im), intent(in) :: fice, hice, & + & tisfc, prsik, prslk + +! --- input/output + real(kind=kind_phys), dimension(im), intent(out) :: cice, zice, & + & tice, work3 + +! --- locals + integer :: i + + do i = 1, im +! transfer ice thickness & concentration from global to local variables + zice(i) = hice(i) + cice(i) = fice(i) + tice(i) = tisfc(i) + work3(i)= prsik(i) / prslk(i) + enddo + + return + end subroutine sfc_sice_pre_run + + end module sfc_sice_pre + + module sfc_sice_post + contains + +! +! \brief This subroutine is empty since there are no procedures needed +! \section arg_table_sfc_sice_post_init Argument Table +! + subroutine sfc_sice_post_init + end subroutine sfc_sice_post_init + +! +! \brief This subroutine is empty since there are no procedures needed +! \section arg_table_sfc_sice_post_finalize Argument Table +! + subroutine sfc_sice_post_finalize + end subroutine sfc_sice_post_finalize + + +! +! \section arg_table_sfc_sice_post_run Argument Table +!! | local var name | longname | description | units | rank | type | kind | intent | optional | +!! |----------------|-------------------------------------------------------|---------------------------------------------|---------------|------|---------|-----------|--------|----------| +!! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | +!! | islmsk | sea_land_ice_mask | sea/land/ice mask (=0/1/2) | flag | 1 | integer | | in | F | +!! | cice | sea_ice_concentration | sea-ice concentration [0,1] | frac | 1 | real | kind_phys | in | F | +!! | zice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kind_phys | in | F | +!! | tice | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kind_phys | in | F | +!! | tsfc | surface_skin_temperature | surface skin temperature | K | 1 | real | kind_phys | in | F | +!! | fice | sea_ice_concentration | sea-ice concentration [0,1] | frac | 1 | real | kind_phys | out | F | +!! | hice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kind_phys | out | F | +!! | tisfc | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kind_phys | out | F | +!! + subroutine sfc_sice_post_run(im, islmsk, cice, zice, tice, tsfc, & + & fice, hice, tisfc) + + use machine, only : kind_phys + + implicit none + +! --- input + integer :: im + integer, dimension(im) :: islmsk + real(kind=kind_phys), dimension(im), intent(in) :: cice, zice, & + & tice, tsfc + +! --- outputs + real(kind=kind_phys), dimension(im), intent(out) :: fice, hice, & + & tisfc + +! --- locals + integer :: i + +!--- return updated ice thickness & concentration to global arrays +! where there is no ice, set temperature to surface skin temperature. + do i = 1, im + + if (islmsk(i) == 2) then + hice(i) = zice(i) + fice(i) = cice(i) + tisfc(i) = tice(i) + else + hice(i) = 0.0 + fice(i) = 0.0 + tisfc(i) = tsfc(i) + endif + enddo + + end subroutine sfc_sice_post_run + + end module sfc_sice_post + + module sfc_sice contains @@ -67,20 +202,19 @@ end subroutine sfc_sice_finalize !! | evap | kinematic_surface_upward_latent_heat_flux | evaporative latent heat flux | kg kg-1 m s-1 | 1 | real | kind_phys | out | F | !! | hflx | kinematic_surface_upward_sensible_heat_flux | kinematic sensible heat flux | K m s-1 | 1 | real | kind_phys | out | F | !! -!! \section general_sice_run General Algorithm +!> \section general_sice_run General Algorithm !! The ice model main program ice3lay() performs two functions: !! - \b Calculation \b of \b ice \b temperature !!\n The surface temperature is determined from the diagnostic balance between !! the upward conduction of heat through snow and/or ice and upward flux of heat !! from the surface. -!! !! - \b Calculation \b of \b ice \b and \b snow \b changes !!\n In addition to calculating ice temperature changes, the ice model must !! also readjust the sizes of the snow and ice layers 1) to accommodate !! mass fluxes at the upper and lower surfaces, 2) to convert snow below !! the water line to ice, and 3) to equalize the thickness of the two !! ice layers. -!! \section detailed_sice_run Detailed Algorithm +!> \section detailed_sice_run Detailed Algorithm !! @{ subroutine sfc_sice_run & & ( im, km, ps, u1, v1, t1, q1, delt, & @@ -184,15 +318,15 @@ subroutine sfc_sice_run & implicit none ! ! - Define constant parameters - integer, parameter :: kmi = 2 !> - 2-layer of ice + integer, parameter :: kmi = 2 !< 2-layer of ice real(kind=kind_phys), parameter :: cpinv = 1.0/cp real(kind=kind_phys), parameter :: hvapi = 1.0/hvap real(kind=kind_phys), parameter :: elocp = hvap/cp - real(kind=kind_phys), parameter :: himax = 8.0 !> - maximum ice thickness allowed - real(kind=kind_phys), parameter :: himin = 0.1 !> - minimum ice thickness required - real(kind=kind_phys), parameter :: hsmax = 2.0 ! maximum snow depth allowed - real(kind=kind_phys), parameter :: timin = 173.0 ! minimum temperature allowed for snow/ice - real(kind=kind_phys), parameter :: albfw = 0.06 ! albedo for lead + real(kind=kind_phys), parameter :: himax = 8.0 !< maximum ice thickness allowed + real(kind=kind_phys), parameter :: himin = 0.1 !< minimum ice thickness required + real(kind=kind_phys), parameter :: hsmax = 2.0 !< maximum snow depth allowed + real(kind=kind_phys), parameter :: timin = 173.0 !< minimum temperature allowed for snow/ice + real(kind=kind_phys), parameter :: albfw = 0.06 !< albedo for lead real(kind=kind_phys), parameter :: dsi = 1.0/0.33 ! --- inputs: @@ -235,7 +369,7 @@ subroutine sfc_sice_run & ! !===> ... begin here ! -! --- ... set flag for sea-ice +!> - Set flag for sea-ice. do i = 1, im flag(i) = (islimsk(i) >= 2) .and. flag_iter(i) @@ -245,7 +379,7 @@ subroutine sfc_sice_run & endif enddo -! --- ... update sea ice temperature +!> - Update/read sea ice temperature from soil temperature and initialize variables. do k = 1, kmi do i = 1, im @@ -334,7 +468,7 @@ subroutine sfc_sice_run & chh(i) = rho(i) * ch(i) * wind rch(i) = chh(i) * cp -! --- ... sensible and latent heat flux over open water & sea ice +!> - Calculate sensible and latent heat flux over open water & sea ice. evapi(i) = elocp * rch(i) * (qssi - q0) evapw(i) = elocp * rch(i) * (qssw - q0) @@ -456,6 +590,7 @@ subroutine sfc_sice_run & enddo ! return +!! @} ! ================= contains @@ -743,7 +878,6 @@ subroutine ice3lay !................................... end subroutine ice3lay !----------------------------------- -!! @} ! =========================== ! ! end contain programs ! @@ -757,139 +891,3 @@ end subroutine sfc_sice_run end module sfc_sice - module sfc_sice_pre - - contains - -! -! \brief This subroutine is empty since there are no procedures needed -! \section arg_table_sfc_sice_pre_init Argument Table -! - subroutine sfc_sice_pre_init - end subroutine sfc_sice_pre_init - -! -! \brief This subroutine is empty since there are no procedures needed -! \section arg_table_sfc_sice_pre_finalize Argument Table -! - subroutine sfc_sice_pre_finalize - end subroutine sfc_sice_pre_finalize - - -! \section arg_table_sfc_sice_pre_run Argument Table -!! | local var name | longname | description | units | rank | type | kind | intent | optional | -!! |----------------|------------------------------------------------------------------------------|-------------------------------------------------------------|---------------|------|---------|-----------|--------|----------| -!! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | -!! | fice | sea_ice_concentration | sea-ice concentration [0,1] | frac | 1 | real | kind_phys | in | F | -!! | hice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kind_phys | in | F | -!! | tisfc | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kind_phys | in | F | -!! | prsik | exner_function_at_lowest_model_interface | Exner function at lowest model interface | none | 1 | real | kind_phys | in | F | -!! | prslk | dimensionless_exner_function_at_lowest_model_layer | dimensionless Exner function at lowest model layer | none | 1 | real | kind_phys | in | F | -!! | cice | sea_ice_concentration | sea-ice concentration [0,1] | frac | 1 | real | kind_phys | out | F | -!! | zice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kind_phys | out | F | -!! | tice | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kind_phys | out | F | -!! | work3 | ratio_of_exner_function_between_midlayer_and_interface_at_lowest_model_layer | Exner function ratio bt midlayer and interface at 1st layer | ratio | 1 | real | kind_phys | out | F | -!! - subroutine sfc_sice_pre_run(im, fice, hice, tisfc , prsik, prslk, & - & cice, zice, tice, work3) - - use machine, only : kind_phys - - implicit none - -! --- inputs - integer :: im - real(kind=kind_phys), dimension(im), intent(in) :: fice, hice, & - & tisfc, prsik, prslk - -! --- input/output - real(kind=kind_phys), dimension(im), intent(out) :: cice, zice, & - & tice, work3 - -! --- locals - integer :: i - - do i = 1, im -! transfer ice thickness & concentration from global to local variables - zice(i) = hice(i) - cice(i) = fice(i) - tice(i) = tisfc(i) - work3(i)= prsik(i) / prslk(i) - enddo - - return - end subroutine sfc_sice_pre_run - - end module sfc_sice_pre - - module sfc_sice_post - - contains - -! -! \brief This subroutine is empty since there are no procedures needed -! \section arg_table_sfc_sice_post_init Argument Table -! - subroutine sfc_sice_post_init - end subroutine sfc_sice_post_init - -! -! \brief This subroutine is empty since there are no procedures needed -! \section arg_table_sfc_sice_post_finalize Argument Table -! - subroutine sfc_sice_post_finalize - end subroutine sfc_sice_post_finalize - - -! -! \section arg_table_sfc_sice_post_run Argument Table -!! | local var name | longname | description | units | rank | type | kind | intent | optional | -!! |----------------|-------------------------------------------------------|---------------------------------------------|---------------|------|---------|-----------|--------|----------| -!! | im | horizontal_loop_extent | horizontal loop extent | count | 0 | integer | | in | F | -!! | islmsk | sea_land_ice_mask | sea/land/ice mask (=0/1/2) | flag | 1 | integer | | in | F | -!! | cice | sea_ice_concentration | sea-ice concentration [0,1] | frac | 1 | real | kind_phys | in | F | -!! | zice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kind_phys | in | F | -!! | tice | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kind_phys | in | F | -!! | tsfc | surface_skin_temperature | surface skin temperature | K | 1 | real | kind_phys | in | F | -!! | fice | sea_ice_concentration | sea-ice concentration [0,1] | frac | 1 | real | kind_phys | out | F | -!! | hice | sea_ice_thickness | sea-ice thickness | m | 1 | real | kind_phys | out | F | -!! | tisfc | sea_ice_temperature | sea-ice surface temperature | K | 1 | real | kind_phys | out | F | -!! - subroutine sfc_sice_post_run(im, islmsk, cice, zice, tice, tsfc, & - & fice, hice, tisfc) - - use machine, only : kind_phys - - implicit none - -! --- input - integer :: im - integer, dimension(im) :: islmsk - real(kind=kind_phys), dimension(im), intent(in) :: cice, zice, & - & tice, tsfc - -! --- outputs - real(kind=kind_phys), dimension(im), intent(out) :: fice, hice, & - & tisfc - -! --- locals - integer :: i - -!--- return updated ice thickness & concentration to global arrays -! where there is no ice, set temperature to surface skin temperature. - do i = 1, im - - if (islmsk(i) == 2) then - hice(i) = zice(i) - fice(i) = cice(i) - tisfc(i) = tice(i) - else - hice(i) = 0.0 - fice(i) = 0.0 - tisfc(i) = tsfc(i) - endif - enddo - - end subroutine sfc_sice_post_run - - end module sfc_sice_post diff --git a/physics/sfcsub.f b/physics/sfcsub.f index 9f4dd1b3d..d13c34fe0 100644 --- a/physics/sfcsub.f +++ b/physics/sfcsub.f @@ -2,8 +2,8 @@ !! This file sets, updates and quility controls numerous surface fields !! such as soil moisture and SST. !! -!!\defgroup static Surface Static Fields -!!\ingroup NOAH +!\defgroup static Surface Static Fields +!\ingroup Noah_Main !!\brief The GFS physics module "sfcsub.f" sets, updates and quality !! controls numerous surface fields such as soil moisture and SST. !! diff --git a/physics/sflx.f b/physics/sflx.f index 113b9b91f..8410815f3 100644 --- a/physics/sflx.f +++ b/physics/sflx.f @@ -1,27 +1,122 @@ !\file sflx.f -!! This file contains the NCEP NOAH LSM (Version 2.7.1) +!! This file is the entity of GFS Noah LSM Model(Version 2.7). -!>\defgroup NOAH_LSM NCEP NOAH LSM -!!\ingroup NOAH_drv -!!\brief This is sub-driver for "NOAH/OSU LSM" family of physics subroutines. +!>\defgroup Noah_LSM GFS Noah LSM Model +!!\ingroup Noah_Main +!!\brief This is the entity of GFS Noah LSM model of physics subroutines. !! It is a soil/veg/snowpack land-surface model to update soil moisture, soil !! ice, soil temperature, skin temperature, snowpack water content, snowdepth, !! and all terms of the surface energy balance and surface water balance -!! (excluding input atmospheric forcings of downward radiation and precip). +!! (excluding input atmospheric forcings of downward radiation \ref RRTMG and +!! precipitation \ref CALPRECIPTYPE). !! -!\section general_sflx General Algorithm +!! The land-surface model component was substantially upgraded from the Oregon +!! State University (OSU) land surface model to EMC's new Noah Land Surface Model +!! (Noah LSM) during the major implementation in the NCEP Global Forecast System +!! (GFS) on May 31, 2005. Forecast System (GFS). The Noah LSM embodies about 10 +!! years of upgrades (see Chen et al. 1996 +!! \cite chen_et_al_1996; Koren et al. 1999 \cite koren_et_al_1999; Ek et al. 2003 +!! \cite ek_et_al_2003) to its ancestor, the OSU LSM. The Noah LSM upgrade includes: +!! - An increase from two (10, 190 cm thick) to four soil layers (10, 30, 60, 100 cm thick) +!! - Addition of frozen soil physics +!! - Add glacial ice treatment +!! - Two snowpack states (SWE, density) +!! - New formulations for infiltration and runoff account for sub-grid variability in precipitation and soil moisture +!! - Revised physics of the snowpack and its influence on surface heat fluxes and albedo +!! - Higher canopy resistance +!! - Spatially varying root depth +!! - Surface fluxes weighted by snow cover fraction +!! - Improved thermal conduction in soil/snow +!! - Improved seasonality of green vegetation cover. +!! - Improved evaporation treatment over bare soil and snowpack +!! +!!\param[in] nsoil integer, number of soil layers (>=2 but <=nsold) +!!\param[in] couple integer, =0:uncoupled (land model only), +!! =1:coupled with parent atmos model +!!\param[in] icein integer, sea-ice flag (=1: sea-ice, =0: land) +!!\param[in] ffrozp real, flag for snow-rain detection (1.=snow, 0.=rain) +!!\param[in] dt real, time step (<3600 sec) +!!\param[in] zlvl real, height abv atmos ground forcing vars (\f$m\f$) +!!\param[in] sldpth real, thickness of each soil layer (\f$m\f$), nsoil +!!\param[in] swdn real, downward SW radiation flux (\f$W/m^2\f$) +!!\param[in] swnet real, downward SW net (dn-up) flux (\f$W/m^2\f$) +!!\param[in] lwdn real, downward LW radiation flux (\f$W/m^2\f$) +!!\param[in] sfcems real, sfc LW emissivity (fractional) +!!\param[in] sfcprs real, pressure at height zlvl above ground(\f$Pa\f$) +!!\param[in] sfctmp real, air temp at height zlvl above ground (\f$K\f$) +!!\param[in] sfcspd real, wind speed at height zlvl above ground (\f$m s^{-1}\f$) +!!\param[in] prcp real, precipitation rate (\f$kgm^{-2}s^{-1}\f$) +!!\param[in] q2 real, mixing ratio at hght zlvl above ground (\f$kgkg^{-1}\f$) +!!\param[in] q2sat real, sat mixing ratio at zlvl above ground (\f$kgkg^{-1}\f$) +!!\param[in] dqsdt2 real, slope of sat specific humidity curve at t=sfctmp (\f$kgkg^{-1}k^{-1}\f$) +!!\param[in] th2 real, air potential temperature at zlvl above ground (\f$K\f$) +!!\param[in] ivegsrc integer, sfc veg type data source UMD or IGBP +!!\param[in] vegtyp integer, vegetation type (integer index) +!!\param[in] soiltyp integer, soil type (integer index) +!!\param[in] slopetyp integer, class of sfc slope (integer index) +!!\param[in] shdmin real, min areal coverage of green veg (fraction) +!!\param[in] alb real, background snow-free sfc albedo (fraction) +!!\param[in] snoalb real, max albedo over deep snow (fraction) +!!\param[in,out] tbot real, bottom soil temp (\f$K\f$) (local yearly-mean sfc air temp) +!!\param[in,out] cmc real, canopy moisture content (\f$m\f$) +!!\param[in,out] t1 real, ground/canopy/snowpack eff skin temp (\f$K\f$) +!!\param[in,out] stc real, soil temp (\f$K\f$) +!!\param[in,out] smc real, total soil moisture (vol fraction) +!!\param[in,out] sh2o real, unfrozen soil moisture (vol fraction), note: frozen part = smc-sh2o +!!\param[in,out] sneqv real, water-equivalent snow depth (\f$m\f$), note: snow density = snwqv/snowh +!!\param[in,out] ch real, sfc exchange coeff for heat & moisture (\f$ms^{-1}\f$), note: conductance since it's been mult by wind +!!\param[in,out] cm real, sfc exchange coeff for momentum (\f$ms^{-1}\f$), note: conductance since it's been mult by wind +!!\param[in,out] z0 real, roughness length (\f$m\f$) +!!\param[out] nroot integer, number of root layers +!!\param[out] shdfac real, aeral coverage of green veg (fraction) +!!\param[out] snowh real, snow depth (\f$m\f$) +!!\param[out] albedo real, sfc albedo incl snow effect (fraction) +!!\param[out] eta real, downward latent heat flux (\f$W/m^2\f$) +!!\param[out] sheat real, downward sensible heat flux (\f$W/m^2\f$) +!!\param[out] ec real, canopy water evaporation (\f$W/m^2\f$) +!!\param[out] edir real, direct soil evaporation (\f$W/m^2\f$) +!!\param[out] et real, plant transpiration (\f$W/m^2\f$) +!!\param[out] ett real, total plant transpiration (\f$W/m^2\f$) +!!\param[out] esnow real, sublimation from snowpack (\f$W/m^2\f$) +!!\param[out] drip real, through-fall of precip and/or dew in excess of canopy water-holding capacity (\f$m\f$) +!!\param[out] dew real, dewfall (or frostfall for t<273.15) (\f$m\f$) +!!\param[out] beta real, ratio of actual/potential evap +!!\param[out] etp real, potential evaporation (\f$W/m^2\f$) +!!\param[out] ssoil real, upward soil heat flux (\f$W/m^2\f$) +!!\param[out] flx1 real, precip-snow sfc flux (\f$W/m^2\f$) +!!\param[out] flx2 real, freezing rain latent heat flux (\f$W/m^2\f$) +!!\param[out] flx3 real, phase-change heat flux from snowmelt (\f$W/m^2\f$) +!!\param[out] runoff1 real, surface runoff (\f$ms^{-1}\f$) not infiltrating sfc +!!\param[out] runoff2 real, sub sfc runoff (\f$ms^{-1}\f$) (baseflow) +!!\param[out] runoff3 real, excess of porosity for a given soil layer +!!\param[out] snomlt real, snow melt (\f$m\f$) (water equivalent) +!!\param[out] sncovr real, fractional snow cover +!!\param[out] rc real, canopy resistance (s/m) +!!\param[out] pc real, plant coeff (fraction) where pc*etp=transpi +!!\param[out] rsmin real, minimum canopy resistance (s/m) +!!\param[out] xlai real, leaf area index (dimensionless) +!!\param[out] rcs real, incoming solar rc factor (dimensionless) +!!\param[out] rct real, air temperature rc factor (dimensionless) +!!\param[out] rcq real, atoms vapor press deficit rc factor +!!\param[out] rcsoil real, soil moisture rc factor (dimensionless) +!!\param[out] soilw real, available soil moisture in root zone +!!\param[out] soilm real, total soil column moisture (frozen+unfrozen) (\f$m\f$) +!!\param[out] smcwlt real, wilting point (volumetric) +!!\param[out] smcdry real, dry soil moisture threshold (volumetric) +!!\param[out] smcref real, soil moisture threshold (volumetric) +!!\param[out] smcmax real, porosity (sat val of soil mois) +!!\section general_sflx General Algorithm +!! @{ !\section detailed_sflx Detailed Algorithm -!----------------------------------- - subroutine sflx & -!................................... -! --- inputs: +! @{ +! subroutine sflx & ! --- inputs: +!ccppdox: avoid to connect to sflx in mpbl + subroutine gfssflx & ! --- inputs: & ( nsoil, couple, icein, ffrozp, dt, zlvl, sldpth, & & swdn, swnet, lwdn, sfcems, sfcprs, sfctmp, & & sfcspd, prcp, q2, q2sat, dqsdt2, th2, ivegsrc, & - & vegtyp, soiltyp, slopetyp, shdmin, alb, snoalb, & -! --- input/outputs: - & tbot, cmc, t1, stc, smc, sh2o, sneqv, ch, cm,z0, & -! --- outputs: + & vegtyp, soiltyp, slopetyp, shdmin, alb, snoalb, & ! --- input/outputs: + & tbot, cmc, t1, stc, smc, sh2o, sneqv, ch, cm,z0, & ! --- outputs: & nroot, shdfac, snowh, albedo, eta, sheat, ec, & & edir, et, ett, esnow, drip, dew, beta, etp, ssoil, & & flx1, flx2, flx3, runoff1, runoff2, runoff3, & @@ -258,7 +353,8 @@ subroutine sflx & ! if vegtype=15 (glacial-ice), re-set ice flag = -1 (glacial-ice) ! note - for open-sea, sflx should *not* have been called. set green ! vegetation fraction (shdfac) = 0. - +!> - For open-sea, sea-ice and glacial-ice cases, sflx() should not have +!! been called (set green vegetation fraction (shdfac) =0.) ice = icein if(ivegsrc == 2) then @@ -275,6 +371,7 @@ subroutine sflx & endif endif +!> - Calculate soil layer depth below ground (sigin of \a zsoil is negative). if (ice == 1) then shdfac = 0.0 @@ -303,6 +400,8 @@ subroutine sflx & ! including soil-type and veg-type dependent parameters. ! set shdfac=0.0 for bare soil surfaces +!> - Call redprm() to set the land-surface paramters, +!! including soil-type and veg-type dependent parameters. call redprm if(ivegsrc == 1) then !only igbp type has urban @@ -331,10 +430,10 @@ subroutine sflx & snowng = .false. frzgra = .false. -! --- ... over sea-ice or glacial-ice, if s.w.e. (sneqv) below threshold -! lower bound (0.01 m for sea-ice, 0.10 m for glacial-ice), then -! set at lower bound and store the source increment in subsurface -! runoff/baseflow (runoff2). +!> - Over sea-ice or glacial-ice, if water-equivalent snow depth (\a sneqv) below threshold +!! lower bound (0.01 m for sea-ice, 0.10 m for glacial-ice), then +!! set at lower bound and store the source increment in subsurface +!! runoff/baseflow (runoff2). ! note - runoff2 is then a negative value (as a flag) over sea-ice or ! glacial-ice, in order to achieve water balance. @@ -358,8 +457,8 @@ subroutine sflx & endif ! end if_ice_block -! --- ... for sea-ice and glacial-ice cases, set smc and sh2o values = 1 -! as a flag for non-soil medium +!> - For sea-ice and glacial-ice cases, set smc and sh2o values = 1.0 +!! as a flag for non-soil medium. if (ice /= 0) then do kz = 1, nsoil @@ -368,9 +467,9 @@ subroutine sflx & enddo endif -! --- ... if input snowpack is nonzero, then compute snow density "sndens" -! and snow thermal conductivity "sncond" (note that csnow is a -! function subroutine) +!> - If input snowpack (\a sneqv) is nonzero, then call csnow() to compute +!! snow density (\a sndens) and snow thermal conductivity (\a sncond). +! (note that csnow is a function subroutine) if (sneqv .eq. 0.0) then sndens = 0.0 @@ -388,10 +487,11 @@ subroutine sflx & endif -! --- ... determine if it's precipitating and what kind of precip it is. -! if it's prcping and the air temp is colder than 0 c, it's snowing! -! if it's prcping and the air temp is warmer than 0 c, but the grnd -! temp is colder than 0 c, freezing rain is presumed to be falling. +!> - Determine if it's precipitating and what kind of precipitation it is. +!! if it's precipitating and the air temperature is colder than \f$0^oC\f$, +!! it's snowing! if it's precipitating and the air temperature is warmer than +!! \f$0^oC\f$, but the ground temperature is colder than \f$0^oC\f$, freezing +!! rain is presumed to be falling. if (prcp > 0.0) then if (ffrozp > 0.5) then @@ -401,11 +501,12 @@ subroutine sflx & endif endif -! --- ... if either prcp flag is set, determine new snowfall (converting -! prcp rate from kg m-2 s-1 to a liquid equiv snow depth in meters) -! and add it to the existing snowpack. -! note - that since all precip is added to snowpack, no precip infiltrates -! into the soil so that prcp1 is set to zero. +!> - If either precipitation flag (\a snowng, \a frzgra) is set as true: +! determine new snowfall (converting precipitation rate from +! \f$kg m^{-2} s^{-1}\f$ to a liquid equiv snow depth in meters) +! and add it to the existing snowpack. +!> - Since all precip is added to snowpack, no precip infiltrates +!! into the soil so that \a prcp1 is set to zero. if (snowng .or. frzgra) then @@ -413,15 +514,15 @@ subroutine sflx & sneqv = sneqv + sn_new prcp1 = 0.0 -! --- ... update snow density based on new snowfall, using old and new -! snow. update snow thermal conductivity - +!> - Call snow_new() to update snow density based on new snowfall, +!! using old and new snow. call snow_new ! --- inputs: ! ! ( sfctmp, sn_new, ! ! --- input/outputs: ! ! snowh, sndens ) ! +!> - Call csnow() to update snow thermal conductivity. call csnow ! --- inputs: ! ! ( sndens, ! @@ -430,15 +531,16 @@ subroutine sflx & else -! --- ... precip is liquid (rain), hence save in the precip variable -! that later can wholely or partially infiltrate the soil (along -! with any canopy "drip" added to this later) +!> - If precipitation is liquid (rain), hence save in the precip variable +!! that later can wholely or partially infiltrate the soil (along +!! with any canopy "drip" added to this later). prcp1 = prcp endif ! end if_snowng_block -! --- ... determine snowcover fraction and albedo fraction over land. +!> - Determine snowcover fraction and albedo fraction over sea-ice, +!! glacial-ice, and land. For nonzero snow depth over land case: if (ice /= 0) then @@ -461,13 +563,15 @@ subroutine sflx & ! --- ... determine snow fraction cover. ! determine surface albedo modification due to snowdepth state. - +!> - Call snfrac() to calculate snow fraction cover. call snfrac ! --- inputs: ! ! ( sneqv, snup, salp, snowh, ! ! --- outputs: ! ! sncovr ) ! +!> - Call alcalc() to calculate surface albedo modification due to snowdepth +!! state. call alcalc ! --- inputs: ! ! ( alb, snoalb, shdfac, shdmin, sncovr, tsnow, ! @@ -479,12 +583,17 @@ subroutine sflx & endif ! end if_ice_block ! --- ... thermal conductivity for sea-ice case, glacial-ice case +!> - Calculate thermal diffusivity (\a df1): +!> - For sea-ice case and glacial-ice case, this is constant(\f$df1=2.2\f$). if (ice /= 0) then df1 = 2.2 else +!> - For non-glacial land case, call tdfcnd() to calculate the thermal +!! diffusivity of top soil layer (Peters-Lidard et al.(1998) +!! \cite peters-lidard_et_al_1998). ! --- ... next calculate the subsurface heat flux, which first requires ! calculation of the thermal diffusivity. treatment of the @@ -510,15 +619,16 @@ subroutine sflx & ! --- outputs: & df1 & & ) +!> - For IGBP/urban, \f$df1=3.24\f$. if(ivegsrc == 1) then !only igbp type has urban !urban if ( vegtyp == 13 ) df1=3.24 endif -! --- ... next add subsurface heat flux reduction effect from the -! overlying green canopy, adapted from section 2.1.2 of -! peters-lidard et al. (1997, jgr, vol 102(d4)) +!> - Add subsurface heat flux reduction effect from the +!! overlying green canopy, adapted from section 2.1.2 of +!! Peters-Lidard et al. (1997) \cite peters-lidard_et_al_1997. df1 = df1 * exp( sbeta*shdfac ) @@ -557,16 +667,16 @@ subroutine sflx & ! df1 = df1h*sncovr + df1 *(1.0-sncovr) df1 = df1a*sncovr + df1 *(1.0-sncovr) -! --- ... calculate subsurface heat flux, ssoil, from final thermal -! diffusivity of surface mediums, df1 above, and skin -! temperature and top mid-layer soil temperature +!> - Calculate subsurface heat flux, \a ssoil, from final thermal +!! diffusivity of surface mediums,\a df1 above, and skin +!! temperature and top mid-layer soil temperature. ssoil = df1 * (t1 - stc(1)) / dtot endif ! end if_sneqv_block -! --- ... determine surface roughness over snowpack using snow condition -! from the previous timestep. +!> - For uncoupled mode, call snowz0() to calculate surface roughness +!! (\a z0) over snowpack using snow condition from the previous timestep. ! if (couple == 0) then ! uncoupled mode if (sncovr > 0.0) then @@ -580,8 +690,8 @@ subroutine sflx & endif ! endif -! --- ... calc virtual temps and virtual potential temps needed by -! subroutines sfcdif and penman. +!> - Calculate virtual temps and virtual potential temps needed by +!! subroutines sfcdif and penman. t2v = sfctmp * (1.0 + 0.61*q2) @@ -611,6 +721,10 @@ subroutine sflx & ! note - fdown, swdn are derived differently in the uncoupled and ! coupled modes. +!> - Calculate the total downward radiation (\a fdown) = net solar (\a swnet) + +!! downward longwave (\a lwdn) as input of penman() and other surface +!! energy budget calculations. + if (couple == 0) then !......uncoupled mode ! --- ... uncoupled mode: @@ -643,9 +757,9 @@ subroutine sflx & endif ! end if_couple_block -! --- ... call penman subroutine to calculate potential evaporation (etp), -! and other partial products and sums save in common/rite for later -! calculations. +!> - Call penman() to calculate potential evaporation (\a etp), +!! and other partial products and sums for later +!! calculations. call penman ! --- inputs: ! @@ -654,8 +768,8 @@ subroutine sflx & ! --- outputs: ! ! t24, etp, rch, epsca, rr, flx2 ) ! -! --- ... call canres to calculate the canopy resistance and convert it -! into pc if nonzero greenness fraction +!> - Call canres() to calculate the canopy resistance and convert it +!! into pc if nonzero greenness fraction. if (shdfac > 0.) then @@ -672,13 +786,15 @@ subroutine sflx & endif -! --- ... now decide major pathway branch to take depending on whether -! snowpack exists or not: +!> - Now decide major pathway branch to take depending on whether +!! snowpack exists or not: esnow = 0.0 if (sneqv .eq. 0.0) then - +!> - For no snowpack is present, call nopac() to calculate soil moisture +!! and heat flux values and update soil moisture contant and soil heat +!! content values. call nopac ! --- inputs: ! ! ( nsoil, nroot, etp, prcp, smcmax, smcwlt, smcref, ! @@ -694,6 +810,7 @@ subroutine sflx & else +!> - For a snowpack is present, call snopac(). call snopac ! --- inputs: ! ! ( nsoil, nroot, etp, prcp, smcmax, smcwlt, smcref, smcdry, ! @@ -709,14 +826,14 @@ subroutine sflx & ! ett, snomlt, drip, dew, flx1, flx3, esnow ) ! endif - -! --- ... prepare sensible heat (h) for return to parent model +!> - Noah LSM post-processing: +!> - Calculate sensible heat (h) for return to parent model. sheat = -(ch*cp1*sfcprs) / (rd1*t2v) * (th2 - t1) -! --- ... convert units and/or sign of total evap (eta), potential evap (etp), -! subsurface heat flux (s), and runoffs for what parent model expects -! convert eta from kg m-2 s-1 to w m-2 +!> - Convert units and/or sign of total evap (eta), potential evap (etp), +!! subsurface heat flux (s), and runoffs for what parent model expects. +! convert eta from kg m-2 s-1 to w m-2 ! eta = eta * lsubc ! etp = etp * lsubc @@ -739,34 +856,34 @@ subroutine sflx & beta = eta / etp -! --- ... convert the sign of soil heat flux so that: -! ssoil>0: warm the surface (night time) -! ssoil<0: cool the surface (day time) +!> - Convert the sign of soil heat flux so that: +!! - ssoil>0: warm the surface (night time) +!! - ssoil<0: cool the surface (day time) ssoil = -1.0 * ssoil if (ice == 0) then -! --- ... for the case of land (but not glacial-ice): -! convert runoff3 (internal layer runoff from supersat) from m -! to m s-1 and add to subsurface runoff/baseflow (runoff2). -! runoff2 is already a rate at this point. +!> - For the case of land (but not glacial-ice): +!! convert runoff3 (internal layer runoff from supersat) from \f$m\f$ +!! to \f$ms^-1\f$ and add to subsurface runoff/baseflow (runoff2). +!! runoff2 is already a rate at this point. runoff3 = runoff3 / dt runoff2 = runoff2 + runoff3 else -! --- ... for the case of sea-ice (ice=1) or glacial-ice (ice=-1), add any -! snowmelt directly to surface runoff (runoff1) since there is no -! soil medium, and thus no call to subroutine smflx (for soil -! moisture tendency). +!> - For the case of sea-ice (ice=1) or glacial-ice (ice=-1), add any +!! snowmelt directly to surface runoff (runoff1) since there is no +!! soil medium, and thus no call to subroutine smflx (for soil +!! moisture tendency). runoff1 = snomlt / dt endif -! --- ... total column soil moisture in meters (soilm) and root-zone -! soil moisture availability (fraction) relative to porosity/saturation +!> - Calculate total column soil moisture in meters (soilm) and root-zone +!! soil moisture availability (fraction) relative to porosity/saturation. soilm = -1.0 * smc(1) * zsoil(1) do k = 2, nsoil @@ -794,7 +911,8 @@ subroutine sflx & !*************************************! !----------------------------------- -!>This subroutine calculates albedo including snow effect (0 -> 1). +!> This subroutine calculates albedo including snow effect (0 -> 1). +!!\ingroup Noah_LSM subroutine alcalc !................................... ! --- inputs: @@ -882,7 +1000,6 @@ end subroutine alcalc !! deficit at the lowest model level, and soil moisture (preferably unfrozen !! soil moisture rather than total). subroutine canres -!................................... ! --- inputs: ! & ( nsoil, nroot, swdn, ch, q2, q2sat, dqsdt2, sfctmp, & ! & sfcprs, sfcems, sh2o, smcwlt, smcref, zsoil, rsmin, & @@ -1099,7 +1216,7 @@ end subroutine csnow !----------------------------------- !> This subroutine calculates soil moisture and heat flux values and !! update soil moisture content and soil heat content values for the -!! case when now snow pack is present. +!! case when no snow pack is present. subroutine nopac !................................... ! --- inputs: @@ -1474,7 +1591,7 @@ end subroutine penman !----------------------------------- !> This subroutine internally sets default values or optionally read-in !! via namelist i/o, all soil and vegetation parateters requied for the execusion -!! of the NOAH LSM. +!! of the Noah LSM. subroutine redprm !................................... ! --- inputs: @@ -5564,6 +5681,7 @@ end subroutine wdfcnd ! =========================== ! 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zZPVquJk}BbbfJ`hKt%U=Pyp3fuh`E~0pH(<{KW|g$j>Ks z7SPgZT8cu$D+0tTGPF{`$bPDoKO0}gzW*q{$g=iDrP5!KJxs4^v`>tlBug072WSy#xZu<0O6i#FAfK{vZ+yn$Y}v~7~CWb%P*-T7`gWRq7C zPVqcz9*t8@p@-<|?xTYU@?Z$BcUR^3pJMNVKgpUg#I-_ERn3Hf8n2 zUaggSFu=y0f7g-@IRw4`bH~pB(!>Jrp&6fpAEN5)epoFlS{m%ae9Uv9eC5Y~1i$c? zr%w{_4ajB%xxczE_;c862!n1C8y8Ee(;rJ=(2-gGA8BR|C!_SnLEjMqY0$K-&cfPD z3)rK-sT)%2sZ$k3O&jn0a;6+IbLu+Rnsff{T4HvZ)_=~wF!gNe`f}Kmp|aq>%Fk)B zQ2W;?W5)6Skqpos?ZZhd`tM=h$=5xqOSjl`ttR{L1$t_*fS;C{zUo_L+lc=I)Vtm* literal 0 HcmV?d00001 From 3bed171b534803d5e332ec34926290582b661515 Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Tue, 6 Mar 2018 14:44:40 -0700 Subject: [PATCH 18/22] add ice3lay doc. --- physics/docs/library.bib | 14 +++++- physics/docs/txt/GFS_NOAH.txt | 4 +- physics/docs/txt/GFS_OZPHYS.txt | 8 ++-- physics/docs/txt/GFS_SFCSICE.txt | 11 +++-- physics/sfc_sice.f | 80 ++++++++++++++++++++++---------- 5 files changed, 81 insertions(+), 36 deletions(-) diff --git a/physics/docs/library.bib b/physics/docs/library.bib index 2f99a8efd..95737121b 100644 --- a/physics/docs/library.bib +++ b/physics/docs/library.bib @@ -1,13 +1,23 @@ %% This BibTeX bibliography file was created using BibDesk. %% http://bibdesk.sourceforge.net/ -%% Created for Man Zhang at 2018-02-26 15:56:22 -0700 +%% Created for Man Zhang at 2018-02-28 08:53:15 -0700 %% Saved with string encoding Unicode (UTF-8) +@inproceedings{untch_et_al_1999, + Author = {A. Untch and A. J. Simmons and M. Hortal and C. Jakob}, + Booktitle = {Proceedings of the SODA Workshop}, + Date-Added = {2018-02-28 15:47:49 +0000}, + Date-Modified = {2018-02-28 15:50:58 +0000}, + Pages = {45-52}, + Publisher = {Netherlands}, + Title = {Increased stratospheric resolution in the ECMWF forecasting system}, + Year = {1999}} + @article{dethof_and_holm_2004, Author = {A. Dethof and E. V. Holm}, Date-Added = {2018-02-26 22:54:54 +0000}, @@ -25,7 +35,7 @@ @techreport{jackson_and_saunders_2002 Institution = {Met Office}, Number = {394}, Title = {Ozone data assimilation: preliminary system}, - Type = {Forecasting Research Technical Report }, + Type = {Forecasting Research Technical Report}, Year = {2002}} @article{riishojgaard_1996, diff --git a/physics/docs/txt/GFS_NOAH.txt b/physics/docs/txt/GFS_NOAH.txt index 6e47d6bc1..5a3ebb3ef 100644 --- a/physics/docs/txt/GFS_NOAH.txt +++ b/physics/docs/txt/GFS_NOAH.txt @@ -42,13 +42,13 @@ Recently, the land surface updates in 2017 GFS operational physics includes: \image html land_dataset.png "Figure 2: Land Data Sets Used in NCEP Modeling Systems" width=10cm -This scheme include the following modules: +This scheme includes the following modules: + \ref Noah_drv + \ref Noah_LSM \section intra_noah 2. Intraphysics Communication + GFS Noah LSM Driver (\ref arg_table_lsm_Noah_run) - + GFS Noah LSM Model (sflx()) + + GFS Noah LSM Model (gfssflx()) \section gen_al_noah 3. General Algorithm + GFS Noah LSM Driver (\ref general_noah_drv) diff --git a/physics/docs/txt/GFS_OZPHYS.txt b/physics/docs/txt/GFS_OZPHYS.txt index 2ae0c5ec9..e45db75e4 100644 --- a/physics/docs/txt/GFS_OZPHYS.txt +++ b/physics/docs/txt/GFS_OZPHYS.txt @@ -4,14 +4,16 @@ In recent years, the leading NWP centers have extended the vertical range of their NWP and DA systems from the surface up through the stratosphere (~10-50 km altitude) and lower mesosphere (~50-65 km). Some have also added stratospheric ozone (\f$O_3\f$) as a prognostic trace constituent to their models. Examples - include the Integrated Forecast System (IFS) of the European Centre for Medium Range Weather Forecasts (ECMWF)(Untch et al., 1999\cite untch_et_al; Dethof and Holm, 2004 \cite dethof_and_holm_2004), and the NCEP GFS (NCEP 2003). The addition + include the Integrated Forecast System (IFS) of the European Centre for Medium Range Weather Forecasts (ECMWF) +(Untch et al., 1999\cite untch_et_al_1999; Dethof and Holm, 2004 \cite dethof_and_holm_2004), and the NCEP GFS (NCEP 2003). The addition of stratospheric ozone as a prognostic variable is expected to improve overall forecast and analyses skill of other fields, such as temperature and wind. The primary reasons for this are: - - more accurate assimilation of satellite radiances from channels that are sensitive to ozone(Derber and Wu, 1998 \cite derber_and_wu_1998; John and Buehler, 2004 \cite john_and_buehler_2004); + - more accurate assimilation of satellite radiances from channels that are sensitive to ozone + (Derber and Wu, 1998 \cite derber_and_wu_1998; John and Buehler, 2004 \cite john_and_buehler_2004); - utilization of correlations between ozone and wind to improve wind analyses in the upper troposphere and lower stratosphere (UTLS) (e.g. Riishojgaard, 1996 \cite riishojgaard_1996); - more accurate radiative heating rates, and hence temperatures arising from using analysed ozone rather than climatological -ozone in the forecast model radiation sheme (often referred to as 'ozone/radiation interaction') (Jackson and Saunders, 2002 \cite jackson_and_saunders_2002); +ozone in the forecast model radiation sheme (often referred to as "ozone/radiation interaction") (Jackson and Saunders, 2002 \cite jackson_and_saunders_2002); - more accurate analyses and forecasts of surface ultraviolet (UV) radiation. With the extension of NWP/DA systems into the upper stratosphere, assimilation and advection alone cannot yield accurate ozone diff --git a/physics/docs/txt/GFS_SFCSICE.txt b/physics/docs/txt/GFS_SFCSICE.txt index d6fdf64b6..4577e6a3f 100644 --- a/physics/docs/txt/GFS_SFCSICE.txt +++ b/physics/docs/txt/GFS_SFCSICE.txt @@ -46,13 +46,16 @@ The model consists of a zero-heat-capacity snow layer overlying two equally thick sea ice layers (Fig.1). The upper ice layer has a variable heat capacity to represent brine pockets. + This scheme includes the following modules: + + \ref GFS_Ice + + Winton(2000) \cite winton_2000 Three-layer Thermodynamics Sea Ice Model ice3lay() \section intra_sice 2. Intraphysics Communication \image html schematic_sice.png "Fig.2 NCEP Sea Ice Model System Diagram" width=10cm -\sa \ref arg_table_sfc_sice_run ++ GFS Sea Ice Driver(\ref arg_table_sfc_sice_run) ++ Winton(2000) \cite winton_2000 Three-layer Thermodynamics Sea Ice Model (ice3lay()) \section gen_sice 3. General Algorithm -\sa \ref general_sice_run - - ++ GFS Sea Ice Driver (\ref general_sice_run) ++ Winton(2000) \cite winton_2000 Three-layer Thermodynamics Sea Ice Model (\ref gen_ice3lay) */ diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index b12a6a39c..16387bcb7 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -361,7 +361,7 @@ subroutine sfc_sice_run & real (kind=kind_phys) :: t12, t14, tem, stsice(im,kmi) &, hflxi, hflxw, q0, qs1, wind, qssi, qssw - real (kind=kind_phys), parameter :: cimin=0.15 ! --- minimum ice concentration + real (kind=kind_phys), parameter :: cimin=0.15 !< minimum ice concentration integer :: i, k @@ -448,7 +448,7 @@ subroutine sfc_sice_run & qssw = fpvs(tgice) qssw = eps*qssw / (ps(i) + epsm1*qssw) -! --- ... snow depth in water equivalent is converted from mm to m unit +!> - Convert snow depth in water equivalent from mm to m unit. if (mom4ice) then snowd(i) = weasd(i) * 0.001 / fice(i) @@ -478,17 +478,17 @@ subroutine sfc_sice_run & snetw(i) = sfcdsw(i) * (1.0 - albfw) snetw(i) = min(3.0*sfcnsw(i)/(1.0+2.0*ffw(i)), snetw(i)) -! - Calculate sneti +!> - Calculate net solar incoming at top \a sneti. sneti(i) = (sfcnsw(i) - ffw(i)*snetw(i)) / fice(i) t12 = tice(i) * tice(i) t14 = t12 * t12 -! - Calculate hfi = net non-solar and upir heat flux @ ice surface +!> - Calculate net non-solar and upir heat flux @ ice surface \a hfi. hfi(i) = -dlwflx(i) + sfcemis(i)*sbc*t14 + evapi(i) & & + rch(i)*(tice(i) - theta1(i)) -! - Calculate hfd +!> - Calculate heat flux derivative at surface \a hfd. hfd(i) = 4.0*sfcemis(i)*sbc*tice(i)*t12 & & + (1.0 + elocp*eps*hvap*qs1/(rd*t12)) * rch(i) @@ -500,9 +500,12 @@ subroutine sfc_sice_run & ! hfw(i) = -dlwflx(i) + sfcemis(i)*sbc*t14 + evapw(i) & ! & + rch(i)*(tgice - theta1(i)) - snetw(i) +!> - Assigin heat flux from ocean \a focn and snowfall rate as constants, which +!! should be from ocean model and other physics. focn(i) = 2.0 ! heat flux from ocean - should be from ocn model snof(i) = 0.0 ! snowfall rate - snow accumulates in gbphys +!> - Initialize snow depth \a snowd. hice(i) = max( min( hice(i), himax ), himin ) snowd(i) = min( snowd(i), hsmax ) @@ -514,6 +517,7 @@ subroutine sfc_sice_run & endif enddo +!> - Call the three-layer thermodynamics sea ice model ice3lay(). ! if (lprnt) write(0,*)' tice2=',tice(ipr) call ice3lay ! --- inputs: ! @@ -611,13 +615,15 @@ subroutine sfc_sice_run & !!\param[in] sneti real, net solar incoming at top (\f$W/m^2\f$) !!\param[in] focn real, heat flux from ocean (\f$W/m^2\f$) !!\param[in] delt real, time step(\f$sec\f$) -!!\param[in,out] snowd real, surface pressure +!!\param[in,out] snowd real, snow depth !!\param[in,out] hice real, sea-ice thickness !!\param[in,out] stsice real, temperature at mid-point of ice levels (\f$^oC\f$) !!\param[in,out] tice real, surface temperature (\f$^oC\f$) !!\param[in,out] snof real, snowfall rate (\f$ms^{-1}\f$) !!\param[out] snowmt real, snow melt during delt (\f$m\f$) !!\param[out] gflux real, conductive heat flux (\f$W/m^2\f$) +!>\section gen_ice3lay General Algorithm +!! @{ subroutine ice3lay !................................... ! --- inputs: @@ -681,23 +687,23 @@ subroutine ice3lay ! ! --- constant parameters: (properties of ice, snow, and seawater) - real (kind=kind_phys), parameter :: ds = 330.0 ! snow (ov sea ice) density (kg/m^3) - real (kind=kind_phys), parameter :: dw =1000.0 ! fresh water density (kg/m^3) + real (kind=kind_phys), parameter :: ds = 330.0 !< snow (ov sea ice) density (kg/m^3) + real (kind=kind_phys), parameter :: dw =1000.0 !< fresh water density (kg/m^3) real (kind=kind_phys), parameter :: dsdw = ds/dw real (kind=kind_phys), parameter :: dwds = dw/ds - real (kind=kind_phys), parameter :: t0c =273.15 ! freezing temp of fresh ice (k) - real (kind=kind_phys), parameter :: ks = 0.31 ! conductivity of snow (w/mk) - real (kind=kind_phys), parameter :: i0 = 0.3 ! ice surface penetrating solar fraction - real (kind=kind_phys), parameter :: ki = 2.03 ! conductivity of ice (w/mk) - real (kind=kind_phys), parameter :: di = 917.0 ! density of ice (kg/m^3) + real (kind=kind_phys), parameter :: t0c =273.15 !< freezing temp of fresh ice (k) + real (kind=kind_phys), parameter :: ks = 0.31 !< conductivity of snow (w/mk) + real (kind=kind_phys), parameter :: i0 = 0.3 !< ice surface penetrating solar fraction + real (kind=kind_phys), parameter :: ki = 2.03 !< conductivity of ice (w/mk) + real (kind=kind_phys), parameter :: di = 917.0 !< density of ice (kg/m^3) real (kind=kind_phys), parameter :: didw = di/dw real (kind=kind_phys), parameter :: dsdi = ds/di - real (kind=kind_phys), parameter :: ci = 2054.0 ! heat capacity of fresh ice (j/kg/k) - real (kind=kind_phys), parameter :: li = 3.34e5 ! latent heat of fusion (j/kg-ice) - real (kind=kind_phys), parameter :: si = 1.0 ! salinity of sea ice - real (kind=kind_phys), parameter :: mu = 0.054 ! relates freezing temp to salinity - real (kind=kind_phys), parameter :: tfi = -mu*si ! sea ice freezing temp = -mu*salinity - real (kind=kind_phys), parameter :: tfw = -1.8 ! tfw - seawater freezing temp (c) + real (kind=kind_phys), parameter :: ci = 2054.0 !< heat capacity of fresh ice (j/kg/k) + real (kind=kind_phys), parameter :: li = 3.34e5 !< latent heat of fusion (j/kg-ice) + real (kind=kind_phys), parameter :: si = 1.0 !< salinity of sea ice + real (kind=kind_phys), parameter :: mu = 0.054 !< relates freezing temp to salinity + real (kind=kind_phys), parameter :: tfi = -mu*si !< sea ice freezing temp = -mu*salinity + real (kind=kind_phys), parameter :: tfw = -1.8 !< tfw - seawater freezing temp (c) real (kind=kind_phys), parameter :: tfi0 = tfi-0.0001 real (kind=kind_phys), parameter :: dici = di*ci real (kind=kind_phys), parameter :: dili = di*li @@ -765,11 +771,17 @@ subroutine ice3lay endif tice(i) = min(tice(i), tsf) -! --- ... compute ice temperature +!> - Ice temperature calculation. bi = hfd(i) ai = hfi(i) - sneti(i) + ip - tice(i)*bi ! +v sol input here +!> - Calculate the effective conductive coupling of the snow-ice layer +!! between the surface and the upper layer ice temperature \f$h_i/4\f$ +!! beneath the snow-ice interface (see \a eq.(5) in Winton(2000) \cite winton_2000). k12 = ki4*ks / (ks*hice(i) + ki4*snowd(i)) + +!> - Calculate the conductive coupling between the two ice temperature +!! points (see \a eq.(10) in Winton(2000) \cite winton_2000). k32 = (ki+ki) / hice(i) wrk = 1.0 / (dt6*k32 + dici*hice(i)) @@ -783,9 +795,18 @@ subroutine ice3lay b1 = b10 + ai * wrk1 c1 = dili * tfi * dt2i * hice(i) +!> - Calculate the new upper ice temperature following \a eq.(21) +!! in Winton(2000) \cite winton_2000. stsice(i,1) = -(sqrt(b1*b1 - 4.0*a1*c1) + b1)/(a1+a1) tice(i) = (k12*stsice(i,1) - ai) / (k12 + bi) +!> - If the surface temperature is greater than the freezing temperature +!! of snow (when there is snow over) or sea ice (when there is none), the +!! surface temperature is fixed at the melting temperature of snow or sea +!! ice, respectively, and the upper ice temperature is recomputed from +!! \a eq.(21) using the coefficients given by \a eqs. (19),(20), and (18). An energy flux +!! \a eq.(22) is applied toward surface melting thereby balancing the surface +!! energy budget. if (tice(i) > tsf) then a1 = a10 + k12 b1 = b10 - k12*tsf @@ -796,18 +817,23 @@ subroutine ice3lay tmelt = 0.0 snowd(i) = snowd(i) + snof(i)*delt endif - +!> - Calculate the new lower ice temperature following \a eq.(15) +!! in Winton(2000) \cite winton_2000. stsice(i,2) = (dt2*k32*(stsice(i,1) + tfw + tfw) & & + dici*hice(i)*stsice(i,2)) * wrk +!> - Calculate the energy for bottom melting (or freezing, if negative) +!! following \a eq.(23), which serves to balance the difference between +!! the oceanic heat flux to the ice bottom and the conductive flux of +!! heat upward from the bottom. bmelt = (focn(i) + ki4*(stsice(i,2) - tfw)/hice(i)) * delt -! --- ... resize the ice ... +!> - Calculation of ice and snow mass changes. h1 = 0.5 * hice(i) h2 = 0.5 * hice(i) -! --- ... top ... +!> - Calculate the top layer thickness. if (tmelt <= snowd(i)*dsli) then snowmt(i) = tmelt / dsli @@ -820,7 +846,9 @@ subroutine ice3lay endif ! --- ... and bottom - +!> - When the energy for bottem melting \f$M_b\f$ is negative (i.e., freezing +!! is happening),calculate the bottom layer thickness \f$h_2\f$ and the new +!! lower layer temperature (see \a eqs.(24)-(26)). if (bmelt < 0.0) then dh = -bmelt / (dili + dici*(tfi - tfw)) stsice(i,2) = (h2*stsice(i,2) + dh*tfw) / (h2 + dh) @@ -829,7 +857,8 @@ subroutine ice3lay h2 = h2 - bmelt / (dili + dici*(tfi - stsice(i,2))) endif -! --- ... if ice remains, even up 2 layers, else, pass negative energy back in snow +!> - If ice remains, even up 2 layers, else, pass negative energy back in snow. +!! Calculate the new upper layer temperature (see \a eq.(38)). hice(i) = h1 + h2 @@ -877,6 +906,7 @@ subroutine ice3lay return !................................... end subroutine ice3lay +!! @} !----------------------------------- ! =========================== ! From 524bf78ee617c51488bef3e21e8f078cfd8400a8 Mon Sep 17 00:00:00 2001 From: "Man.Zhang" Date: Wed, 7 Mar 2018 08:40:37 -0700 Subject: [PATCH 19/22] fix bugs --- physics/ozphys.f | 7 +++---- physics/sflx.f | 2 +- 2 files changed, 4 insertions(+), 5 deletions(-) diff --git a/physics/ozphys.f b/physics/ozphys.f index ce431711b..22cd13ba2 100644 --- a/physics/ozphys.f +++ b/physics/ozphys.f @@ -68,10 +68,9 @@ end subroutine ozphys_init !! !! \section genal_ozphys General Algorithm !> @{ - subroutine ozphys_run ( & - & ix, im, levs, ko3, dt, ozi, ozo, tin, po3,& - & prsl, prdout, pl_coeff, delp, ldiag3d,& - & ozp, me) + subroutine ozphys_run (ix, im, levs, ko3, dt, ozi, ozo, tin, po3, & + & prsl, prdout, pl_coeff, delp, ldiag3d, & + & ozp, me) ! ! this code assumes that both prsl and po3 are from bottom to top ! as are all other variables diff --git a/physics/sflx.f b/physics/sflx.f index 8410815f3..c523ca3da 100644 --- a/physics/sflx.f +++ b/physics/sflx.f @@ -111,7 +111,7 @@ ! @{ ! subroutine sflx & ! --- inputs: !ccppdox: avoid to connect to sflx in mpbl - subroutine gfssflx & ! --- inputs: + subroutine gfssflx & ! --- inputs: & ( nsoil, couple, icein, ffrozp, dt, zlvl, sldpth, & & swdn, swnet, lwdn, sfcems, sfcprs, sfctmp, & & sfcspd, prcp, q2, q2sat, dqsdt2, th2, ivegsrc, & From 12300f515be270384085438d231c85eb6244339d Mon Sep 17 00:00:00 2001 From: "Man.Zhang" Date: Fri, 9 Mar 2018 10:55:47 -0700 Subject: [PATCH 20/22] minor changes to fix warnings --- physics/docs/ccpp_dox | 2 ++ physics/docs/txt/GFS_GWDC.txt | 2 +- physics/docs/txt/GFS_SFCLYR.txt | 2 +- physics/mfdeepcnv.f | 4 +++- physics/mfshalcnv.f | 3 --- physics/module_nst_model.f90 | 1 - physics/sfc_diff.f | 2 -- physics/sfc_sice.f | 32 ++++++++++++++++---------------- physics/sflx.f | 3 --- 9 files changed, 23 insertions(+), 28 deletions(-) diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index a93ba6d43..82868c1e4 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -140,6 +140,7 @@ INPUT = txt/mainpage_bootstrapped.txt \ ../sfc_drv.f \ ../sflx.f \ ../sfc_diff.f \ + ../GFS_calpreciptype.f90 \ ### Sea Ice Surface ../sfc_sice.f \ ### Ocean Surface @@ -156,6 +157,7 @@ INPUT = txt/mainpage_bootstrapped.txt \ ../ozphys.f \ INPUT_ENCODING = UTF-8 FILE_PATTERNS = *.f \ + *.f90 \ *.txt RECURSIVE = YES EXCLUDE = diff --git a/physics/docs/txt/GFS_GWDC.txt b/physics/docs/txt/GFS_GWDC.txt index 128c95dd0..6183f4896 100644 --- a/physics/docs/txt/GFS_GWDC.txt +++ b/physics/docs/txt/GFS_GWDC.txt @@ -24,7 +24,7 @@ the stable stratosphere can generate gravity waves that influence the large-scale flow. - \image html GFS_gwdc.png "Figure 1: Gravity waves generated by penetrative convection in the presence of background wind. (Based on Hooke(1986) \cite hooke_1986; and Kim et al. (2003) \cite kim_et_al_2003)" width=10cm + \image html GFS_gwdc.png "Figure 1: Gravity waves generated by penetrative convection in the presence of background wind. (Based on Hooke(1986); and Kim et al. (2003))" width=10cm Compared with orographic gravitity waves, it has proven more difficult to model the way in which gravity waves are generated by various convective sources; The simplest situation is depicted in diff --git a/physics/docs/txt/GFS_SFCLYR.txt b/physics/docs/txt/GFS_SFCLYR.txt index 7daae3adf..8e58730f0 100644 --- a/physics/docs/txt/GFS_SFCLYR.txt +++ b/physics/docs/txt/GFS_SFCLYR.txt @@ -5,7 +5,7 @@ the surface sublayer scheme from Zeng and Dickinson (1998) \cite zeng_and_dickinson_1998. - \ref NOAH are largely responsible for the quality + \ref Noah_Main are largely responsible for the quality of model forecasts produced for near-surface weather parameters, such as 2-meter air temperature (\f$T_{2m}\f$) and surface skin temperature (\f$LST\f$). \f$LST\f$ is derived from the surface energy budget, and is diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 4dbb0e4a6..17bb37f86 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -1,6 +1,7 @@ !> \file mfdeepcnv.f !! This file contains the entire SAMF deep convection scheme. !> \defgroup SAMF GFS Scale-Aware Mass-Flux Deep Convection +!> @{ !> \brief The scale-aware mass-flux (SAMF) deep convection scheme is an !! updated version of the previous Simplified Arakawa-Schubert (SAS) scheme !! with scale and aerosol awareness and parameterizes the effect of deep @@ -70,8 +71,8 @@ subroutine sasasdeep_finalize end subroutine sasasdeep_finalize !>\defgroup GFS_mfdeep GFS mfdeepcnv Main +!! @{ !!\ingroup SAMF -!> @{ !>\brief This subroutine contains the entirety of the SAMF deep convection scheme. !! !! For grid sizes larger than threshold value, as in Grell (1993) @@ -2657,5 +2658,6 @@ subroutine sasasdeep_run(im,ix,km,delt,delp,prslp,psp,phil,ql1, & return !! @} end subroutine sasasdeep_run +!! @} !> @} end module sasas_deep diff --git a/physics/mfshalcnv.f b/physics/mfshalcnv.f index 815de6e75..17282ca50 100644 --- a/physics/mfshalcnv.f +++ b/physics/mfshalcnv.f @@ -95,7 +95,6 @@ end subroutine sasasshal_finalize !> \defgroup SAMF_shal GFS Scale-Aware Mass-Flux Shallow Convection -!> @{ !! \brief The scale-aware mass-flux shallow (SAMF_shal) convection !! scheme is an updated version of the previous mass-flux shallow !! convection scheme with scale and aerosol awareness and @@ -1785,7 +1784,5 @@ subroutine sasasshal_run (im,ix,km,delt,delp,prslp,psp,phil,ql1, & !! @} end subroutine sasasshal_run !! @} -!> @} - end module sasas_shal diff --git a/physics/module_nst_model.f90 b/physics/module_nst_model.f90 index a5c31808f..978a642dc 100644 --- a/physics/module_nst_model.f90 +++ b/physics/module_nst_model.f90 @@ -937,6 +937,5 @@ subroutine dtl_reset(xt,xs,xu,xv,xz,xzts,xtts) xzts = 0.0 end subroutine dtl_reset - end module nst_module !! @ } diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index 0376357e5..ec44fad04 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -79,7 +79,6 @@ end subroutine sfc_ex_coef_finalize !!\f] !! -# Calculate the exchange coefficients:\f$cm\f$, \f$ch\f$, and \f$stress\f$ as inputs of other \a sfc schemes. !! \section detailed_diff Detailed Algorithm -!! !! @{ subroutine sfc_ex_coef_run & & (im,ps,u1,v1,t1,q1,z1, & @@ -397,5 +396,4 @@ subroutine sfc_ex_coef_run & return end subroutine sfc_ex_coef_run !! @} - end module surface_exchange_coefficients diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 16387bcb7..f46f91495 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -606,22 +606,22 @@ subroutine sfc_sice_run & !! based on Winton(2000) \cite winton_2000 . !! @{ !!\ingroup gfs_sice_main -!!\param[in] im integer, horizontal dimension -!!\param[in] kmi integer, number of ice layers (2) -!!\param[in] fice real, sea-ice concentration -!!\param[in] flag logical, ice mask flag -!!\param[in] hfi real, net non-solar and heat flux at surface (\f$W/m^2\f$) -!!\param[in] hfd real, heat flux derivative at surface -!!\param[in] sneti real, net solar incoming at top (\f$W/m^2\f$) -!!\param[in] focn real, heat flux from ocean (\f$W/m^2\f$) -!!\param[in] delt real, time step(\f$sec\f$) -!!\param[in,out] snowd real, snow depth -!!\param[in,out] hice real, sea-ice thickness -!!\param[in,out] stsice real, temperature at mid-point of ice levels (\f$^oC\f$) -!!\param[in,out] tice real, surface temperature (\f$^oC\f$) -!!\param[in,out] snof real, snowfall rate (\f$ms^{-1}\f$) -!!\param[out] snowmt real, snow melt during delt (\f$m\f$) -!!\param[out] gflux real, conductive heat flux (\f$W/m^2\f$) +!\param[in] im integer, horizontal dimension +!\param[in] kmi integer, number of ice layers (2) +!\param[in] fice real, sea-ice concentration +!\param[in] flag logical, ice mask flag +!\param[in] hfi real, net non-solar and heat flux at surface (\f$W/m^2\f$) +!\param[in] hfd real, heat flux derivative at surface +!\param[in] sneti real, net solar incoming at top (\f$W/m^2\f$) +!\param[in] focn real, heat flux from ocean (\f$W/m^2\f$) +!\param[in] delt real, time step(\f$sec\f$) +!\param[in,out] snowd real, snow depth +!\param[in,out] hice real, sea-ice thickness +!\param[in,out] stsice real, temperature at mid-point of ice levels (\f$^oC\f$) +!\param[in,out] tice real, surface temperature (\f$^oC\f$) +!\param[in,out] snof real, snowfall rate (\f$ms^{-1}\f$) +!\param[out] snowmt real, snow melt during delt (\f$m\f$) +!\param[out] gflux real, conductive heat flux (\f$W/m^2\f$) !>\section gen_ice3lay General Algorithm !! @{ subroutine ice3lay diff --git a/physics/sflx.f b/physics/sflx.f index c523ca3da..e329d5d94 100644 --- a/physics/sflx.f +++ b/physics/sflx.f @@ -107,8 +107,6 @@ !!\param[out] smcmax real, porosity (sat val of soil mois) !!\section general_sflx General Algorithm !! @{ -!\section detailed_sflx Detailed Algorithm -! @{ ! subroutine sflx & ! --- inputs: !ccppdox: avoid to connect to sflx in mpbl subroutine gfssflx & ! --- inputs: @@ -5684,4 +5682,3 @@ end subroutine wdfcnd end subroutine gfssflx !----------------------------------- !! @} - From 596acf0e7d6c4bcb0480ab3e4a874f79d4a74a4a Mon Sep 17 00:00:00 2001 From: "Man.Zhang" Date: Wed, 14 Mar 2018 17:03:16 -0600 Subject: [PATCH 21/22] some txt fix per Ligia's comments. --- physics/docs/txt/GFS_GWDC.txt | 6 +++--- physics/docs/txt/GFS_GWDPS.txt | 6 +++--- physics/docs/txt/GFS_HEDMF.txt | 6 +++--- physics/docs/txt/GFS_NSST.txt | 4 ++-- physics/docs/txt/GFS_OZPHYS.txt | 4 ++-- physics/docs/txt/GFS_RAYLEIGH.txt | 2 +- physics/docs/txt/GFS_RRTMG.txt | 8 ++++---- physics/docs/txt/GFS_SAMFdeep.txt | 8 +++----- physics/docs/txt/GFS_SAMFshal.txt | 6 +++--- physics/docs/txt/GFS_SFCLYR.txt | 4 ++-- physics/docs/txt/mainpage_bootstrapped.txt | 10 ++++------ 11 files changed, 30 insertions(+), 34 deletions(-) diff --git a/physics/docs/txt/GFS_GWDC.txt b/physics/docs/txt/GFS_GWDC.txt index 6183f4896..bcc523e89 100644 --- a/physics/docs/txt/GFS_GWDC.txt +++ b/physics/docs/txt/GFS_GWDC.txt @@ -39,13 +39,13 @@ is activated in a conditionally unstable atmosphere. \section intra_gwdc 2. Intraphysics Communication -\sa \ref arg_table_gwdc_run +\ref arg_table_gwdc_run \section gena_gwdc 3. General Algorithm -\sa \ref gen_gwdc +\ref gen_gwdc \section det_gwdc 4. Detailed Algorithm -\sa \ref al_gwdc +\ref al_gwdc diff --git a/physics/docs/txt/GFS_GWDPS.txt b/physics/docs/txt/GFS_GWDPS.txt index 20b400aa1..87af93b59 100644 --- a/physics/docs/txt/GFS_GWDPS.txt +++ b/physics/docs/txt/GFS_GWDPS.txt @@ -92,13 +92,13 @@ \section intra_gwdps 2. Intraphysics Communication -\sa \ref arg_table_gwdps_run +\ref arg_table_gwdps_run \section gen_al_gwdps 3. General Algorithm -\sa \ref gen_gwdps +\ref gen_gwdps \section detailed_al_gwdps 4. Detailed Algorithm -\sa \ref det_gwdps +\ref det_gwdps */ diff --git a/physics/docs/txt/GFS_HEDMF.txt b/physics/docs/txt/GFS_HEDMF.txt index b0e03ea95..07aff21fa 100644 --- a/physics/docs/txt/GFS_HEDMF.txt +++ b/physics/docs/txt/GFS_HEDMF.txt @@ -14,13 +14,13 @@ This scheme includes the following subroutines: + mfpbl() \section intra_pbl 2. Intraphysics Communication -\sa \ref arg_table_edmf_run +\ref arg_table_edmf_run \section gen_pbl 3. General Algorithm -\sa \ref general_edmf +\ref general_edmf \section det_pbl 4. Detailed Algorithm -\sa \ref detailed_edmf +\ref detailed_edmf diff --git a/physics/docs/txt/GFS_NSST.txt b/physics/docs/txt/GFS_NSST.txt index ab255f262..9c0939b1e 100644 --- a/physics/docs/txt/GFS_NSST.txt +++ b/physics/docs/txt/GFS_NSST.txt @@ -27,10 +27,10 @@ This scheme includes the following components: + \ref nst_parameters \section intra_nst 2. Intraphysics Communication -\sa \ref arg_table_sfc_nst_run +\ref arg_table_sfc_nst_run \section gen_nst 3. General Algorithm -\sa \ref NSST_general_algorithm +\ref NSST_general_algorithm */ diff --git a/physics/docs/txt/GFS_OZPHYS.txt b/physics/docs/txt/GFS_OZPHYS.txt index e45db75e4..7edea28a2 100644 --- a/physics/docs/txt/GFS_OZPHYS.txt +++ b/physics/docs/txt/GFS_OZPHYS.txt @@ -52,10 +52,10 @@ ozone in the forecast model radiation sheme (often referred to as "ozone/radiati \section intra_ozone 2. Intraphysics Communication -\sa \ref arg_table_ozphys_run +\ref arg_table_ozphys_run \section gen_ozone 3. General Algorithm -\sa \ref genal_ozphys +\ref genal_ozphys diff --git a/physics/docs/txt/GFS_RAYLEIGH.txt b/physics/docs/txt/GFS_RAYLEIGH.txt index 3ba0e093f..1d40b3913 100644 --- a/physics/docs/txt/GFS_RAYLEIGH.txt +++ b/physics/docs/txt/GFS_RAYLEIGH.txt @@ -7,7 +7,7 @@ This is the Rayleigh friction calculation with total energy conservation. - The winter-summer zonal wind drag in the strato-mesosphere \section intra_rayleigh 2. Intraphysics Communication -\sa \ref arg_table_rayleigh_damp_run +\ref arg_table_rayleigh_damp_run \section gen_ozone 3. General Algorithm diff --git a/physics/docs/txt/GFS_RRTMG.txt b/physics/docs/txt/GFS_RRTMG.txt index 7e3c3dca0..f1076a197 100644 --- a/physics/docs/txt/GFS_RRTMG.txt +++ b/physics/docs/txt/GFS_RRTMG.txt @@ -101,12 +101,12 @@ value is used in the upper atmosphere. \section intraphysics_rrtmg 2. Intraphysics Communication - + For RRTMG-Longwave radiation parameterization: \sa \ref arg_table_lwrad_run - + For RRTMG-Shortwave radiation parameterization: \sa \ref arg_table_swrad_run + + For RRTMG-Longwave radiation parameterization: \ref arg_table_lwrad_run + + For RRTMG-Shortwave radiation parameterization: \ref arg_table_swrad_run \section gen_al_rrtmg 3. General Algorithm - + For RRTMG-Longwave radiation parameterization: \sa \ref gen_lwrad - + For RRTMG-Shortwave radiation parameterization: \sa \ref gen_swrad + + For RRTMG-Longwave radiation parameterization: \ref gen_lwrad + + For RRTMG-Shortwave radiation parameterization: \ref gen_swrad */ diff --git a/physics/docs/txt/GFS_SAMFdeep.txt b/physics/docs/txt/GFS_SAMFdeep.txt index 3180e8f3d..bb928a234 100644 --- a/physics/docs/txt/GFS_SAMFdeep.txt +++ b/physics/docs/txt/GFS_SAMFdeep.txt @@ -52,15 +52,13 @@ to more strongly suppress convection in a drier environment. \section intra_deep 2. Intraphysics Communication -\sa \ref arg_table_sasasdeep_run +\ref arg_table_sasasdeep_run \section gen_al_deep 3. General Algorithm -\sa \ref general_mfdeep +\ref general_mfdeep \section det_al_deep 4. Detailed Algorithm -\sa \ref detailed_deep +\ref detailed_deep - - */ diff --git a/physics/docs/txt/GFS_SAMFshal.txt b/physics/docs/txt/GFS_SAMFshal.txt index e5337fe25..efa873e2d 100644 --- a/physics/docs/txt/GFS_SAMFshal.txt +++ b/physics/docs/txt/GFS_SAMFshal.txt @@ -23,13 +23,13 @@ are described in Han et al. (2017) \cite han_et_al_2017 . \section intr_shal 2. Intraphysics Communication -\sa \ref arg_table_sasasshal_run +\ref arg_table_sasasshal_run \section gen_shal 3. General Algorithm -\sa \ref general_mfshal +\ref general_mfshal \section det_shal 4. Detailed Algorithm -\sa \ref detailed_mfshal +\ref detailed_mfshal diff --git a/physics/docs/txt/GFS_SFCLYR.txt b/physics/docs/txt/GFS_SFCLYR.txt index 8e58730f0..b33a0ad92 100644 --- a/physics/docs/txt/GFS_SFCLYR.txt +++ b/physics/docs/txt/GFS_SFCLYR.txt @@ -59,10 +59,10 @@ The daytime \f$LST\f$ increases substantially and is very close to the observations. \section intra_rough 2. Intraphysics Communication -\sa \ref arg_table_sfc_ex_coef_run +\ref arg_table_sfc_ex_coef_run \section gen_rough 3. General Algorithm -\sa \ref general_diff +\ref general_diff diff --git a/physics/docs/txt/mainpage_bootstrapped.txt b/physics/docs/txt/mainpage_bootstrapped.txt index 883304d94..651d4da04 100644 --- a/physics/docs/txt/mainpage_bootstrapped.txt +++ b/physics/docs/txt/mainpage_bootstrapped.txt @@ -4,13 +4,11 @@ \anchor mainpage-top -Welcome to the GMTB Common Community Physics Package (CCPP) documentation for \b the \b 2017 \b Operational \b GFS \b physics \b suite. In this website you will find documentation on various aspects of the 2017 operational GFS physics, including basic description, input/output augument list and general/detailed algorithm. +Welcome to the GMTB Common Community Physics Package (CCPP) V1 documentation. This version contains all parameterizations of \b the \b 2017 \b Operational \b GFS \b physics \b suite. In this website you will find documentation on various aspects of the parameterizations, including basic description, input/output argument list and general/detailed algorithm. -\author Global Model Test Bed (GMTB) at DTC and NOAA/ESRL +\author Global Model Test Bed (GMTB) at NCAR and NOAA/GSD -\copyright GMTB - -Documentation for the individual physics scheme can of 2017 operational GFS physics suite be access through the following links: +Documentation for the individual physics scheme can be accessed through the following links: + @ref GFS_RRTMG + @ref GFS_SAMFdeep + @ref GFS_SAMFshal @@ -25,7 +23,7 @@ Documentation for the individual physics scheme can of 2017 operational GFS phys + @ref GFS_OZPHYS You can find more information about -GMTB Interoperable Physics Driver/Common Community Physics Package(IPD/CCPP) on DTC website +the GMTB Interoperable Physics Driver/Common Community Physics Package(IPD/CCPP) on the DTC website. From ae650ea4989bff8d2f4f4b2bb080eb66bc735758 Mon Sep 17 00:00:00 2001 From: Man Zhang Date: Wed, 14 Mar 2018 20:31:37 -0600 Subject: [PATCH 22/22] get rid of group diagram as Ligia's request. and some doc fix in SAMF-DEEP. --- physics/docs/ccpp_dox | 6 ++-- physics/mfdeepcnv.f | 76 +++++++++++++++++++++---------------------- 2 files changed, 41 insertions(+), 41 deletions(-) diff --git a/physics/docs/ccpp_dox b/physics/docs/ccpp_dox index 82868c1e4..bd3da90b7 100644 --- a/physics/docs/ccpp_dox +++ b/physics/docs/ccpp_dox @@ -302,7 +302,7 @@ ALLEXTERNALS = NO EXTERNAL_GROUPS = YES EXTERNAL_PAGES = YES PERL_PATH = /usr/bin/perl -CLASS_DIAGRAMS = NO +CLASS_DIAGRAMS = YES MSCGEN_PATH = DIA_PATH = HIDE_UNDOC_RELATIONS = YES @@ -312,8 +312,8 @@ DOT_FONTNAME = Helvetica DOT_FONTSIZE = 10 DOT_FONTPATH = CLASS_GRAPH = YES -COLLABORATION_GRAPH = NO -GROUP_GRAPHS = YES +COLLABORATION_GRAPH = YES +GROUP_GRAPHS = NO UML_LOOK = NO UML_LIMIT_NUM_FIELDS = 10 TEMPLATE_RELATIONS = NO diff --git a/physics/mfdeepcnv.f b/physics/mfdeepcnv.f index 17bb37f86..3a59b79be 100644 --- a/physics/mfdeepcnv.f +++ b/physics/mfdeepcnv.f @@ -1,35 +1,53 @@ !> \file mfdeepcnv.f -!! This file contains the entire SAMF deep convection scheme. +!! This file contains the entire scale-aware mass-flux (SAMF) +!! deep convection scheme. + + module sasas_deep + contains + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasdeep_init Argument Table + subroutine sasasdeep_init + end subroutine sasasdeep_init + + +! \brief Brief description of the subroutine +! +! \section arg_table_sasasdeep_finalize Argument Table + subroutine sasasdeep_finalize + end subroutine sasasdeep_finalize + !> \defgroup SAMF GFS Scale-Aware Mass-Flux Deep Convection !> @{ -!> \brief The scale-aware mass-flux (SAMF) deep convection scheme is an -!! updated version of the previous Simplified Arakawa-Schubert (SAS) scheme -!! with scale and aerosol awareness and parameterizes the effect of deep -!! convection on the environment (represented by the model state variables) +!> \brief The scale-aware mass-flux (SAMF) deep convection scheme is an +!! updated version of the previous Simplified Arakawa-Schubert (SAS) scheme +!! with scale and aerosol awareness and parameterizes the effect of deep +!! convection on the environment (represented by the model state variables) !! in the following way. First, a simple cloud model is used to determine -!! the change in model state variables due to one entraining/detraining cloud -!! type, per unit cloud-base mass flux. Next, the total change in state variables -!! is retrieved by determining the actual cloud base mass flux using the -!! quasi-equilibrium assumption (for grid sizes larger than a threshold value -!! [currently set to 8 km]) or a mean updraft velocity (for grid sizes smaller -!! than the threshold value). With a scale-aware parameterization, the -!! cloud mass flux decreases with increasing grid resolution. A simple -!! aerosol-aware parameterization is employed, where rain conversion in -!! the convective updraft is modified by aerosol number concentration. -!! The name SAS is replaced with SAMF as for the smaller grid sizes, -!! the parameterization does not use Arakawa-Schubert's quasi-equilibrium -!! assumption any longer where the cloud work function (interpreted as -!! entrainment-moderated convective available potential energy [CAPE]) +!! the change in model state variables due to one entraining/detraining cloud +!! type, per unit cloud-base mass flux. Next, the total change in state variables +!! is retrieved by determining the actual cloud base mass flux using the +!! quasi-equilibrium assumption (for grid sizes larger than a threshold value +!! [currently set to 8 km]) or a mean updraft velocity (for grid sizes smaller +!! than the threshold value). With a scale-aware parameterization, the +!! cloud mass flux decreases with increasing grid resolution. A simple +!! aerosol-aware parameterization is employed, where rain conversion in +!! the convective updraft is modified by aerosol number concentration. +!! The name SAS is replaced with SAMF as for the smaller grid sizes, +!! the parameterization does not use Arakawa-Schubert's quasi-equilibrium +!! assumption any longer where the cloud work function (interpreted as +!! entrainment-moderated convective available potential energy [CAPE]) !! by the large scale dynamics is in balance with the consumption of the !! cloud work function by the convection. !! -!! The SAS scheme uses the working concepts put forth in Arakawa and +!! The SAS scheme uses the working concepts put forth in Arakawa and !! Schubert (1974) \cite arakawa_and_schubert_1974 but includes modifications !! and simplifications from Grell (1993) \cite grell_1993 such as saturated !! downdrafts and only one cloud type (the deepest possible), rather than !! a spectrum based on cloud top heights or assumed entrainment rates. !! The scheme was implemented for the GFS in 1995 by Pan and Wu -!! \cite pan_and_wu_1995, with further modifications discussed in +!! \cite pan_and_wu_1995, with further modifications discussed in !! Han and Pan (2011) \cite han_and_pan_2011 , including the calculation !! of cloud top, a greater CFL-criterion-based maximum cloud base mass flux, !! updated cloud model entrainment and detrainment, improved convective @@ -52,24 +70,6 @@ !! cloud condensate in the updraft. The lateral entrainment is also enhanced !! to more strongly suppress convection in a drier environment. !! - - - module sasas_deep - contains - -! \brief Brief description of the subroutine -! -! \section arg_table_sasasdeep_init Argument Table - subroutine sasasdeep_init - end subroutine sasasdeep_init - - -! \brief Brief description of the subroutine -! -! \section arg_table_sasasdeep_finalize Argument Table - subroutine sasasdeep_finalize - end subroutine sasasdeep_finalize - !>\defgroup GFS_mfdeep GFS mfdeepcnv Main !! @{ !!\ingroup SAMF