A fully-implicit multi-phase flow model which assumes immiscibility of the phases. More...

#include <opm/material/densead/Math.hpp>
#include "immiscibleproperties.hh"
#include "immiscibleindices.hh"
#include "immiscibleextensivequantities.hh"
#include "immiscibleprimaryvariables.hh"
#include "immiscibleintensivequantities.hh"
#include "immiscibleratevector.hh"
#include "immiscibleboundaryratevector.hh"
#include "immisciblelocalresidual.hh"
#include <opm/models/common/multiphasebasemodel.hh>
#include <opm/models/common/energymodule.hh>
#include <opm/models/io/vtkenergymodule.hpp>
#include <opm/material/components/NullComponent.hpp>
#include <opm/material/fluidsystems/GasPhase.hpp>
#include <opm/material/fluidsystems/LiquidPhase.hpp>
#include <opm/material/fluidsystems/SinglePhaseFluidSystem.hpp>
#include <opm/material/fluidsystems/TwoPhaseImmiscibleFluidSystem.hpp>
#include <sstream>
#include <string>

Classes
class	Opm::ImmiscibleModel< TypeTag >
	A fully-implicit multi-phase flow model which assumes immiscibility of the phases. More...

struct	Opm::Properties::TTag::ImmiscibleModel
	The generic type tag for problems using the immiscible multi-phase model. More...

struct	Opm::Properties::TTag::ImmiscibleSinglePhaseModel
	The type tag for single-phase immiscible problems. More...

struct	Opm::Properties::TTag::ImmiscibleTwoPhaseModel
	The type tag for two-phase immiscible problems. More...

struct	Opm::Properties::LocalResidual< TypeTag, TTag::ImmiscibleModel >
	Use the immiscible multi-phase local jacobian operator for the immiscible multi-phase model. More...

struct	Opm::Properties::Model< TypeTag, TTag::ImmiscibleModel >
	the Model property More...

struct	Opm::Properties::RateVector< TypeTag, TTag::ImmiscibleModel >
	the RateVector property More...

struct	Opm::Properties::BoundaryRateVector< TypeTag, TTag::ImmiscibleModel >
	the BoundaryRateVector property More...

struct	Opm::Properties::PrimaryVariables< TypeTag, TTag::ImmiscibleModel >
	the PrimaryVariables property More...

struct	Opm::Properties::IntensiveQuantities< TypeTag, TTag::ImmiscibleModel >
	the IntensiveQuantities property More...

struct	Opm::Properties::ExtensiveQuantities< TypeTag, TTag::ImmiscibleModel >
	the ExtensiveQuantities property More...

struct	Opm::Properties::Indices< TypeTag, TTag::ImmiscibleModel >
	The indices required by the isothermal immiscible multi-phase model. More...

struct	Opm::Properties::EnableEnergy< TypeTag, TTag::ImmiscibleModel >
	Disable the energy equation by default. More...

struct	Opm::Properties::FluidSystem< TypeTag, TTag::ImmiscibleSinglePhaseModel >
	The fluid system to use by default. More...

struct	Opm::Properties::Fluid< TypeTag, TTag::ImmiscibleSinglePhaseModel >

struct	Opm::Properties::WettingPhase< TypeTag, TTag::ImmiscibleTwoPhaseModel >

struct	Opm::Properties::NonwettingPhase< TypeTag, TTag::ImmiscibleTwoPhaseModel >

struct	Opm::Properties::FluidSystem< TypeTag, TTag::ImmiscibleTwoPhaseModel >

class	Opm::ImmiscibleModel< TypeTag >
	A fully-implicit multi-phase flow model which assumes immiscibility of the phases. More...

Namespaces
	Opm
	Structs needed for tpfalinearizer and its gpuparams struct extracted to be defined in one place that both can include.

	Opm::Properties::TTag
	The generic type tag for problems using the immiscible multi-phase model.

Detailed Description

A fully-implicit multi-phase flow model which assumes immiscibility of the phases.

This model implements multi-phase flow of $M > 0$ immiscible fluids $\alpha$ . By default, the standard multi-phase Darcy approach is used to determine the velocity, i.e.

$\mathbf{v}_\alpha = - \frac{k_{r\alpha}}{\mu_\alpha} \mathbf{K}\left(\mathbf{grad}\, p_\alpha - \varrho_{\alpha} \mathbf{g} \right) \;,$

although the actual approach which is used can be specified via the FluxModule property. For example, the velocity model can by changed to the Forchheimer approach by

template<class TypeTag>

struct FluxModule<TypeTag, TTag::MyProblemTypeTag> { using type = Opm::ForchheimerFluxModule<TypeTag>; };

The core of the model is the conservation mass of each component by means of the equation

$\frac{\partial\;\phi S_\alpha \rho_\alpha }{\partial t} - \mathrm{div} \left\{ \rho_\alpha \mathbf{v}_\alpha \right\} - q_\alpha = 0 \;.$

The model uses the following primary variables:

The pressure in Pascal of the phase with the lowest index
The saturations $S_\alpha$ of the phases that exhibit the lowest indices
The absolute temperature in Kelvin if energy is conserved via the energy equation

Classes

Namespaces

Detailed Description