{ volScalarField divPhi ( "divPhi", fvc::div(phi) ); // Momentum equation fvVectorMatrix UEqn ( fvm::div(phi, U) + turbulence->divDevReff(U) ); // Add MRF sources mrfZones.addCoriolis(UEqn); // Add porous sources tmp tTU; if (addPorosity) { tTU = tmp ( new volTensorField ( IOobject ( "TU", runTime.timeName(), mesh, IOobject::NO_READ, IOobject::NO_WRITE ), mesh, dimensionedTensor("zero", dimless/dimTime, tensor::zero) ) ); volTensorField& TU = tTU(); pZones.addResistance(UEqn, TU); trTU = inv(TU + tensor(I)*UEqn.A()); trTU().rename("rAU"); } else { trAU = 1.0/UEqn.A(); trAU().rename("rAU"); } // Insert the additional components. Note this will destroy the H and A UEqn += fvm::SuSp(-divPhi, U) + divPhi*U; UEqn.relax(); // Insert momentum equation UpEqn.insertEquation(0, UEqn); if (addPorosity) { // Manually over-ride the 3x3 block to handle the off-diagonal // part of the Ap coefficient const tensorField& TUIn = tTU().internalField(); CoeffField::squareTypeField& DD = UpEqn.diag().asSquare(); const scalarField& V = mesh.V().field(); // Note: this insertion should only happen in porous cell zones // A rewrite of the porousZones class interface is needed. // HJ, 14/Mar/2016 forAll (TUIn, cellI) { const scalar& cellV = V[cellI]; const tensor& cellTU = TUIn[cellI]; CoeffField::squareType& cellDD = DD[cellI]; cellDD(0, 0) += cellV*cellTU.xx(); cellDD(0, 1) += cellV*cellTU.xy(); cellDD(0, 2) += cellV*cellTU.xz(); cellDD(1, 0) += cellV*cellTU.yx(); cellDD(1, 1) += cellV*cellTU.yy(); cellDD(2, 2) += cellV*cellTU.yz(); cellDD(2, 0) += cellV*cellTU.zx(); cellDD(2, 1) += cellV*cellTU.zy(); cellDD(2, 2) += cellV*cellTU.zz(); } } }