EEqn.H
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1{
3
4 fvScalarMatrix EEqn
5 (
6 fvm::ddt(rho, he) + mvConvection->fvmDiv(phi, he)
7 + fvc::ddt(rho, K) + fvc::div(phi, K)
8 + (
9 he.name() == "e"
10 ? fvc::div
11 (
12 fvc::absolute(phi/fvc::interpolate(rho), U),
13 p,
14 "div(phiv,p)"
15 )
16 : -dpdt
17 )
18 - fvm::laplacian(turbulence->alphaEff(), he)
19 ==
20 Qdot
21 + fvOptions(rho, he)
22 );
23
24 EEqn.relax();
25
26 fvOptions.constrain(EEqn);
27
28 EEqn.solve();
29
30 fvOptions.correct(he);
31
32 thermo.correct();
33
34 Info<< "min/max(T) = "
35 << min(T).value() << ", " << max(T).value() << endl;
36}
CGAL::Exact_predicates_exact_constructions_kernel K
Y[inertIndex] max(0.0)
volScalarField & he
Definition: YEEqn.H:52
tmp< fv::convectionScheme< scalar > > mvConvection(fv::convectionScheme< scalar >::New(mesh, fields, phi, mesh.divScheme("div(phi,Yi_h)")))
fv::options & fvOptions
surfaceScalarField & phi
Basic thermodynamics type based on the use of fitting functions for cp, h, s obtained from the templa...
U
Definition: pEqn.H:72
volScalarField & p
const volScalarField & T
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))
volScalarField & dpdt
compressible::turbulenceModel & turbulence
GeometricField< scalar, fvPatchField, volMesh > volScalarField
Definition: volFieldsFwd.H:82
scalar Qdot
Definition: solveChemistry.H:2