Richards flow. More...
This model implements a variant of the Richards' equation for quasi-twophase flow.
In the unsaturated zone, Richards' equation is frequently used to approximate the water distribution above the groundwater level (in the unsaturated zone):
\[ \frac{\partial (\phi S_w \varrho_w)}{\partial t} - \nabla \cdot \left\lbrace \varrho_w \frac{k_{rw}}{\mu_w} \; \mathbf{K} \; \left( \nabla p_w - \varrho_w \textbf{g} \right) \right\rbrace = q_w, \]
where:
It can be derived from the two-phase flow equations. In contrast to the full two-phase model, the Richards model assumes gas as the nonwetting fluid and that it exhibits a much lower viscosity than the (liquid) wetting phase. (For example at atmospheric pressure and at room temperature, the viscosity of air is only about \(1\%\) of the viscosity of liquid water.) As a consequence, the mobility ( \(\frac{k_{r}}{\mu}\)) is typically much larger for the gas phase than for the wetting phase. For this reason, the Richards model assumes that gas phase mobility is infinitely large. This implies that the pressure of the gas phase is equivalent to the static pressure distribution and that therefore, mass conservation only needs to be considered for the wetting phase.
The model thus chooses the absolute pressure of the wetting phase \(p_w\) as its only primary variable. The wetting phase saturation is calculated using the inverse of the capillary pressure, i.e.
\[ S_w = p_c^{-1}(p_g - p_w) \]
holds, where \(p_g\) is a given reference gas pressure. Nota bene, that the last step is assumes that the capillary pressure-saturation curve can be uniquely inverted, so it is not possible to set the capillary pressure to zero when using the Richards model!
Files | |
file | porousmediumflow/richards/balanceequationopts.hh |
Traits class to set options used by the local residual when when evaluating the balance equations. | |
file | porousmediumflow/richards/indices.hh |
Index names for the Richards model. | |
file | porousmediumflow/richards/iofields.hh |
Adds I/O fields specific to the Richards model. | |
file | porousmediumflow/richards/localresidual.hh |
Element-wise calculation of the Jacobian matrix for problems using the Richards fully implicit models. | |
file | porousmediumflow/richards/model.hh |
This model implements a variant of the Richards' equation for quasi-twophase flow. | |
file | porousmediumflow/richards/newtonsolver.hh |
A Richards model Newton solver. | |
file | porousmediumflow/richards/velocityoutput.hh |
Velocity output for the Richards model. | |
file | porousmediumflow/richards/volumevariables.hh |
Volume averaged quantities required by the Richards model. | |
Classes | |
struct | Dumux::RichardsBalanceEquationOptions< FluidSystem > |
Traits class to set options used by the local residual when when evaluating the balance equations. More... | |
struct | Dumux::RichardsIndices |
Index names for the Richards model. More... | |
class | Dumux::RichardsIOFields |
Adds I/O fields specific to the Richards model. More... | |
class | Dumux::RichardsLocalResidual< TypeTag > |
Element-wise calculation of the Jacobian matrix for problems using the Richards fully implicit models. More... | |
struct | Dumux::RichardsModelTraits |
Specifies a number properties of the Richards model. More... | |
struct | Dumux::RichardsVolumeVariablesTraits< PV, FSY, FST, SSY, SST, PT, MT > |
Traits class for the Richards model. More... | |
class | Dumux::RichardsNewtonSolver< Assembler, LinearSolver, Reassembler, Comm > |
A Richards model specific Newton solver. More... | |
class | Dumux::RichardsVelocityOutput< GridVariables, FluxVariables > |
Velocity output policy for the Richards model. More... | |
class | Dumux::RichardsVolumeVariables< Traits > |
Volume averaged quantities required by the Richards model. More... | |
struct | Dumux::ExtendedRichardsVolumeVariablesTraits< PV, FSY, FST, SSY, SST, PT, MT, DT, EDM > |
Traits class for the Richards model. More... | |
class | Dumux::ExtendedRichardsPrimaryVariableSwitch |
The primary variable switch controlling the phase presence state variable. More... | |