Go to the source code of this file.
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tmp< fv::convectionScheme< scalar > > | mvConvection (fv::convectionScheme< scalar >::New(mesh, fields, phi, mesh.divScheme("div(phi,Yi_h)"))) |
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combustion | correct () |
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volScalarField | Yt (0.0 *Y[0]) |
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| forAll (Y, i) |
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Y [inertIndex] | max (0.0) |
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fvScalarMatrix | EEqn (fvm::ddt(rho, he)+mvConvection->fvmDiv(phi, he)+fvc::ddt(rho, K)+fvc::div(phi, K)+(he.name()=="e" ? fvc::div(fvc::absolute(phi/fvc::interpolate(rho), U), p, "div(phiv,p)") :-dpdt) - fvm::laplacian(turbulence->alphaEff(), he)==Qdot+radiation->Sh(thermo, he)+parcels.Sh(he)+surfaceFilm.Sh()+fvOptions(rho, he)) |
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EEqn | relax () |
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fvOptions | constrain (EEqn) |
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EEqn | solve () |
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fvOptions | correct (he) |
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◆ mvConvection()
tmp<fv::convectionScheme<scalar> > mvConvection |
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fv::convectionScheme< scalar > |
::Newmesh, fields, phi, mesh.divScheme("div(phi,Yi_h)") | ) |
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◆ correct() [1/2]
◆ Yt()
volScalarField Yt |
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0.0 * |
Y[0] | ) |
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◆ forAll()
Definition at line 17 of file YEEqn.H.
References combustion(), composition, Foam::fvc::ddt(), fvOptions, inertIndex(), Foam::fvc::laplacian(), mesh, mvConvection(), phi, rho, surfaceFilm, turbulence, Y, and Yt().
◆ max()
◆ EEqn()
fvScalarMatrix EEqn |
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fvm::ddt(rho, he)+mvConvection->fvmDiv(phi, he)+fvc::ddt(rho, K)+fvc::div(phi, K)+(he.name()=="e" ? fvc::div(fvc::absolute(phi/fvc::interpolate(rho), U), p, "div(phiv,p)") :-dpdt) - fvm::laplacian(turbulence->alphaEff(), he) |
= =Qdot+radiation->Sh(thermo, he)+parcels.Sh(he)+surfaceFilm.Sh()+fvOptions(rho, he) | ) |
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◆ relax()
◆ constrain()
◆ solve()
◆ correct() [2/2]
◆ Qdot
◆ he
volScalarField& he = thermo.he() |
Definition at line 51 of file YEEqn.H.
Referenced by interRegionHeatTransferModel::addSup(), heThermo< BasicSolidThermo, MixtureType >::he(), heThermo< BasicSolidThermo, MixtureType >::heBoundaryCorrection(), basicThermo::lookupThermo(), radiationModel::radiation(), thermo< Thermo, Type >::typeName(), basicThermo::validate(), and limitTemperature::~limitTemperature().