9 ? fvc::div(
phi, volScalarField(
"Ekp", 0.5*magSqr(
U) +
p/
rho))
10 : fvc::div(
phi, volScalarField(
"K", 0.5*magSqr(
U)))
31 Info<<
"T gas min/max = " << min(
T).value() <<
", "
32 << max(
T).value() << endl;
tmp< fv::convectionScheme< scalar > > mvConvection(fv::convectionScheme< scalar >::New(mesh, fields, phi, mesh.divScheme("div(phi,Yi_h)")))
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))
const uniformDimensionedVectorField & g
Basic thermodynamics type based on the use of fitting functions for cp, h, s obtained from the templa...
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+fvOptions(rho, he))
autoPtr< radiation::radiationModel > radiation(radiation::radiationModel::New(T))
compressible::turbulenceModel & turbulence
GeometricField< scalar, fvPatchField, volMesh > volScalarField