24#ifndef DUMUX_MATERIAL_THERMALCONDUCTIVITY_SOMERTON_3P_HH
25#define DUMUX_MATERIAL_THERMALCONDUCTIVITY_SOMERTON_3P_HH
64class ThermalConductivitySomerton
79 template<
class VolumeVariables>
82 using FluidSystem =
typename VolumeVariables::FluidSystem;
84 const Scalar sw = volVars.saturation(FluidSystem::wPhaseIdx);
85 const Scalar sn = volVars.saturation(FluidSystem::nPhaseIdx);
86 const Scalar lambdaW = volVars.fluidThermalConductivity(FluidSystem::wPhaseIdx);
87 const Scalar lambdaN = volVars.fluidThermalConductivity(FluidSystem::nPhaseIdx);
88 const Scalar lambdaG = volVars.fluidThermalConductivity(FluidSystem::gPhaseIdx);
89 const Scalar lambdaSolid = volVars.solidThermalConductivity();
90 const Scalar
porosity = volVars.porosity();
110 const Scalar lambdaW,
111 const Scalar lambdaN,
112 const Scalar lambdaG,
113 const Scalar lambdaSolid,
119 const Scalar satW = max<Scalar>(0.0, sw);
120 const Scalar satN = max<Scalar>(0.0, sn);
123 const Scalar lSw = pow(lambdaSolid, (1.0 -
porosity)) * pow(lambdaW,
porosity);
124 const Scalar lSn = pow(lambdaSolid, (1.0 -
porosity)) * pow(lambdaN,
porosity);
125 const Scalar lSg = pow(lambdaSolid, (1.0 -
porosity)) * pow(lambdaG,
porosity);
126 const Scalar lambdaEff = lSg + sqrt(satW) * (lSw - lSg) + sqrt(satN) * (lSn -lSg);
Adaption of the non-isothermal two-phase two-component flow model to problems with CO2.
Definition: adapt.hh:29
std::string porosity() noexcept
I/O name of porosity.
Definition: name.hh:139
static Scalar effectiveThermalConductivity(const VolumeVariables &volVars)
effective thermal conductivity after Somerton (1974) extended for a three phase system
Definition: thermalconductivitysomerton3p.hh:80
static Scalar effectiveThermalConductivity(const Scalar sw, const Scalar sn, const Scalar lambdaW, const Scalar lambdaN, const Scalar lambdaG, const Scalar lambdaSolid, const Scalar porosity)
effective thermal conductivity after Somerton (1974)
Definition: thermalconductivitysomerton3p.hh:108