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Copy file name to clipboardExpand all lines: doc/modelling/binding/freundlich_ldf.rst
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@@ -13,9 +13,10 @@ This variant of the model is based on the linear driving force approximation (se
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No interaction between the components is considered when the model has multiple components.
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One of the limitation of this isotherm is the first order Jacobian :math:`\left(\frac{dq^*}{dc_p}\right)` tends to infinity as :math:`c_{p} \rightarrow0` for :math:`n>1`.
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To address this issue an approximation of isotherm is considered near the origin.
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This approximation matches the isotherm in such a way that :math:`q=0` at :math:`c_p=0` and also matches the first derivative of the isotherm at :math:`c_p = \varepsilon`, where :math:`\varepsilon` is a very small number, for example :math:`1e-14`.
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The form of approximation and its derivative is given below for :math:`c_p < \varepsilon` and :math:`n>1`:
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Additionally, the isotherm is undefined for :math:`c_{p} < 0` if :math:`\frac{1}{n_i}` can be expressed as :math:`\frac{p}{q}` with :math:`p,q \in\mathbb{N}` where :math:`q` is an even number.
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To address these issues an approximation of the isotherm is considered below a threshold concentration :math:`c_p < \varepsilon`.
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This approximation matches the isotherm in such a way that :math:`q=0` at :math:`c_p=0` and also matches the value and the first derivative of the isotherm at :math:`c_p = \varepsilon`, where :math:`\varepsilon` is a very small number, for example :math:`1e-14`.
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The form of approximation and its derivative is given below for :math:`c_p < \varepsilon`:
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.. math::
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@@ -39,6 +40,5 @@ where :math:`\alpha_0=0` and :math:`\alpha_1` and :math:`\alpha_2` are determine
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\end{aligned}
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This approximation can be used for any pore phase concentration :math:`c_p < \varepsilon` given :math:`n>1`.
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For the case, when :math:`n \le1` no special treatment near the origin is required.
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For more information on model parameters required to define in CADET file format, see :ref:`freundlich_ldf_config`.
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