/*---------------------------------------------------------------------------*\ ========= | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox \\ / O peration | \\ / A nd | Copyright held by original author \\/ M anipulation | ------------------------------------------------------------------------------- License This file is part of OpenFOAM. OpenFOAM is free software; you can redistribute it and/or modify it under the terms of the GNU General Public License as published by the Free Software Foundation; either version 2 of the License, or (at your option) any later version. OpenFOAM is distributed in the hope that it will be useful, but WITHOUT ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public License for more details. You should have received a copy of the GNU General Public License along with OpenFOAM; if not, write to the Free Software Foundation, Inc., 59 Temple Place, Suite 330, Boston, MA 02111-1307 USA Application PDRFoam Description Compressible premixed/partially-premixed combustion solver with turbulence modelling. Combusting RANS code using the b-Xi two-equation model. Xi may be obtained by either the solution of the Xi transport equation or from an algebraic exression. Both approaches are based on Gulder's flame speed correlation which has been shown to be appropriate by comparison with the results from the spectral model. Strain effects are encorporated directly into the Xi equation but not in the algebraic approximation. Further work need to be done on this issue, particularly regarding the enhanced removal rate caused by flame compression. Analysis using results of the spectral model will be required. For cases involving very lean Propane flames or other flames which are very strain-sensitive, a transport equation for the laminar flame speed is present. This equation is derived using heuristic arguments involving the strain time scale and the strain-rate at extinction. the transport velocity is the same as that for the Xi equation. For large flames e.g. explosions additional modelling for the flame wrinkling due to surface instabilities may be applied. PDR (porosity/distributed resistance) modelling is included to handle regions containing blockages which cannot be resolved by the mesh. \*---------------------------------------------------------------------------*/ #include "fvCFD.H" #include "dynamicFvMesh.H" #include "hhuCombustionThermo.H" #include "RASModel.H" #include "laminarFlameSpeed.H" #include "XiModel.H" #include "PDRDragModel.H" #include "ignition.H" #include "Switch.H" #include "bound.H" #include "dynamicRefineFvMesh.H" // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // int main(int argc, char *argv[]) { # include "setRootCase.H" # include "createTime.H" # include "createDynamicFvMesh.H" # include "readCombustionProperties.H" # include "readEnvironmentalProperties.H" # include "createFields.H" # include "readPISOControls.H" # include "initContinuityErrs.H" # include "readTimeControls.H" # include "setInitialDeltaT.H" scalar StCoNum = 0.0; // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // Info<< "\nStarting time loop\n" << endl; while (runTime.run()) { # include "readTimeControls.H" # include "readPISOControls.H" # include "CourantNo.H" # include "setDeltaT.H" runTime++; Info<< "\n\nTime = " << runTime.timeName() << endl; // Indicators for refinement. Note: before runTime++ // only for postprocessing reasons. tmp tmagGradP = mag(fvc::grad(p)); volScalarField normalisedGradP ( "normalisedGradP", tmagGradP()/max(tmagGradP()) ); normalisedGradP.writeOpt() = IOobject::AUTO_WRITE; tmagGradP.clear(); bool meshChanged = false; { // Make the fluxes absolute fvc::makeAbsolute(phi, rho, U); // Test : disable refinement for some cells PackedList<1>& protectedCell = refCast(mesh).protectedCell(); if (protectedCell.size() == 0) { protectedCell.setSize(mesh.nCells()); protectedCell = 0; } forAll(betav, cellI) { if (betav[cellI] < 0.99) { protectedCell[cellI] = 1; } } //volScalarField pIndicator("pIndicator", // p*(fvc::laplacian(p)) // / ( // magSqr(fvc::grad(p)) // + dimensionedScalar // ( // "smallish", // sqr(p.dimensions()/dimLength), // 1E-6 // ) // )); //pIndicator.writeOpt() = IOobject::AUTO_WRITE; // Flux estimate for introduced faces. volVectorField rhoU("rhoU", rho*U); // Do any mesh changes meshChanged = mesh.update(); // if (mesh.moving() || meshChanged) // { //# include "correctPhi.H" // } // Make the fluxes relative to the mesh motion fvc::makeRelative(phi, rho, U); } # include "rhoEqn.H" # include "UEqn.H" // --- PISO loop for (int corr=1; corr<=nCorr; corr++) { # include "bEqn.H" # include "ftEqn.H" # include "huEqn.H" # include "hEqn.H" if (!ign.ignited()) { hu == h; } # include "pEqn.H" } turbulence->correct(); runTime.write(); Info<< "\nExecutionTime = " << runTime.elapsedCpuTime() << " s\n" << endl; } Info<< "\n end\n"; return(0); } // ************************************************************************* //