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Go to the source code of this file.
Functions | |
| fvScalarMatrix | EEqn (fvm::div(phi, he)+(he.name()=="e" ? fvc::div(phi, volScalarField("Ekp", 0.5 *magSqr(U)+p/rho)) :fvc::div(phi, volScalarField("K", 0.5 *magSqr(U)))) - fvm::laplacian(turbulencePtr_->alphaEff(), he) - fvSourceEnergy - fvOptions(rho, he)) |
| EEqn | relax () |
| fvOptions | constrain (EEqn) |
| thermo | correct () |
Variables | |
| volScalarField & | he = thermo.he() |
| SolverPerformance< scalar > | solverE = EEqn.solve() |
Function Documentation
◆ EEqn()
| fvScalarMatrix EEqn | ( | fvm::div(phi, he)+(he.name()=="e" ? fvc::div(phi, volScalarField("Ekp", 0.5 *magSqr(U)+p/rho)) :fvc::div(phi, volScalarField("K", 0.5 *magSqr(U)))) - fvm::laplacian(turbulencePtr_->alphaEff(), he) - fvSourceEnergy - fvOptions(rho, he) | ) |
◆ relax()
| EEqn relax | ( | ) |
◆ constrain()
| fvOptions constrain | ( | EEqn | ) |
◆ correct()
| thermo correct | ( | ) |
Variable Documentation
◆ he
| volScalarField& he = thermo.he() |
Definition at line 5 of file EEqnRhoSimple.H.
◆ solverE
| SolverPerformance<scalar> solverE = EEqn.solve() |
Definition at line 22 of file EEqnRhoSimple.H.
