{ volScalarField rUrelA = 1.0/UrelEqn.A(); surfaceScalarField psisf = fvc::interpolate(psis); surfaceScalarField rhof = fvc::interpolate(rho); // Needs to be outside of loop since p is changing, but psi and rho are not surfaceScalarField rhoReff = rhof - psisf*fvc::interpolate(p); // --- PISO loop for (int corr = 0; corr < nCorr; corr++) { Urel = rUrelA*UrelEqn.H(); // Calculate phi for boundary conditions phi = rhof*fvc::interpolate(Urel) & mesh.Sf(); surfaceScalarField phid2 = rhoReff/rhof*phi; surfaceScalarField phid("phid", psisf/rhof*phi); p.storePrevIter(); volScalarField divPhid ( "divPhid", fvc::div(phid) ); for (int nonOrth = 0; nonOrth <= nNonOrthCorr; nonOrth++) { fvScalarMatrix pEqn ( fvm::ddt(psis, p) + fvm::div(phid, p) // Convective flux relaxation terms + fvm::SuSp(-divPhid, p) + divPhid*p + fvc::div(phid2) - fvm::laplacian(rho*rUrelA, p) ); // Retain the residual from the first pressure solution eqnResidual = pEqn.solve().initialResidual(); if (corr == 0 && nonOrth == 0) { maxResidual = max(eqnResidual, maxResidual); } // Calculate the flux if (nonOrth == nNonOrthCorr) { phi = phid2 + pEqn.flux(); } } # include "compressibleContinuityErrs.H" // Relax the pressure p.relax(); Urel -= rUrelA*fvc::grad(p); Urel.correctBoundaryConditions(); } // Bound the pressure if (min(p) < pMin || max(p) > pMax) { p.max(pMin); p.min(pMax); p.correctBoundaryConditions(); } // Bound the velocity volScalarField magUrel = mag(Urel); if (max(magUrel) > UrelMax) { volScalarField Urellimiter = pos(magUrel - UrelMax)*UrelMax/(magUrel + smallUrel) + neg(magUrel - UrelMax); Urellimiter.max(scalar(0)); Urellimiter.min(scalar(1)); Urel *= Urellimiter; Urel.correctBoundaryConditions(); } }