Newer
Older
rho1 = eos1->rho(p, T);
rho2 = eos2->rho(p, T);
Henry
committed
volScalarField rAU("rAU", 1.0/UEqn.A());
surfaceScalarField rAUf("Dp", fvc::interpolate(rAU));
volVectorField HbyA("HbyA", U);
HbyA = rAU*UEqn.H();
surfaceScalarField phiHbyA
(
"phiHbyA",
(fvc::interpolate(HbyA) & mesh.Sf())
+ fvc::ddtPhiCorr(rAU, rho, U, phi)
);
phi = phiHbyA;
surfaceScalarField phig
(
(
fvc::interpolate(interface.sigmaK())*fvc::snGrad(alpha1)
- ghf*fvc::snGrad(rho)
)*rAUf*mesh.magSf()
);
phiHbyA += phig;
tmp<fvScalarMatrix> p_rghEqnComp1;
tmp<fvScalarMatrix> p_rghEqnComp2;
//if (transonic)
//{
//}
//else
surfaceScalarField phid1("phid1", fvc::interpolate(psi1)*phi);
surfaceScalarField phid2("phid2", fvc::interpolate(psi2)*phi);
p_rghEqnComp1 =
fvc::ddt(rho1) + psi1*correction(fvm::ddt(p_rgh))
+ fvc::div(phid1, p_rgh)
- fvc::Sp(fvc::div(phid1), p_rgh);
p_rghEqnComp2 =
fvc::ddt(rho2) + psi2*correction(fvm::ddt(p_rgh))
+ fvc::div(phid2, p_rgh)
- fvc::Sp(fvc::div(phid2), p_rgh);
}
// Thermodynamic density needs to be updated by psi*d(p) after the
// pressure solution - done in 2 parts. Part 1:
//thermo.rho() -= psi*p_rgh;
while (pimple.correctNonOrthogonal())
fvScalarMatrix p_rghEqnIncomp
Henry
committed
fvc::div(phiHbyA)
);
solve
(
(
(max(alpha1, scalar(0))/rho1)*p_rghEqnComp1()
+ (max(alpha2, scalar(0))/rho2)*p_rghEqnComp2()
mesh.solver(p_rgh.select(pimple.finalInnerIter()))
);
if (pimple.finalNonOrthogonalIter())
// Second part of thermodynamic density update
//thermo.rho() += psi*p_rgh;
dgdt =
(
pos(alpha2)*(p_rghEqnComp2 & p_rgh)/rho2
- pos(alpha1)*(p_rghEqnComp1 & p_rgh)/rho1
);
Henry
committed
phi = phiHbyA + p_rghEqnIncomp.flux();
U = HbyA
+ rAU*fvc::reconstruct((phig + p_rghEqnIncomp.flux())/rAUf);
U.correctBoundaryConditions();
}
}
p = max(p_rgh + (alpha1*rho1 + alpha2*rho2)*gh, pMin);
rho1 = eos1->rho(p, T);
rho2 = eos2->rho(p, T);
Info<< "max(U) " << max(mag(U)).value() << endl;
Info<< "min(p_rgh) " << min(p_rgh).value() << endl;