simpeg/docs/api_Richards.rst

.. _api_Richards:

There are two different forms of Richards equation that differ
on how they deal with the non-linearity in the time-stepping term.

The most fundamental form, referred to as the
'mixed'-form of Richards Equation [Celia et al., 1990]

.. math::

    \\frac{\partial \\theta(\psi)}{\partial t} - \\nabla \cdot k(\psi) \\nabla \psi - \\frac{\partial k(\psi)}{\partial z} = 0
    \quad \psi \in \Omega

where theta is water content, and psi is pressure head.
This formulation of Richards equation is called the
'mixed'-form because the equation is parameterized in psi
but the time-stepping is in terms of theta.

As noted in [Celia et al., 1990] the 'head'-based form of Richards
equation can be written in the continuous form as:

.. math::

    \\frac{\partial \\theta}{\partial \psi}\\frac{\partial \psi}{\partial t} - \\nabla \cdot k(\psi) \\nabla \psi - \\frac{\partial k(\psi)}{\partial z} = 0
    \quad \psi \in \Omega

However, it can be shown that this does not conserve mass in the discrete formulation.



Richards
========

.. automodule:: simpegFLOW.Richards
    :show-inheritance:
    :members:
    :undoc-members:
    :inherited-members: