/*---------------------------------------------------------------------------*\ ========= | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox \\ / O peration | \\ / A nd | www.openfoam.com \\/ M anipulation | ------------------------------------------------------------------------------- Copyright (C) 2011-2015 OpenFOAM Foundation Copyright (C) 2015-2016 OpenCFD Ltd. ------------------------------------------------------------------------------- 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 3 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, see . Application XiFoam Group grpCombustionSolvers grpMovingMeshSolvers Description Solver for compressible premixed/partially-premixed combustion 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 expression. 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. \*---------------------------------------------------------------------------*/ #include "fvCFD.H" #include "dynamicFvMesh.H" #include "psiuReactionThermo.H" #include "turbulentFluidThermoModel.H" #include "laminarFlameSpeed.H" #include "ignition.H" #include "Switch.H" #include "pimpleControl.H" #include "CorrectPhi.H" #include "fvOptions.H" // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // int main(int argc, char *argv[]) { argList::addNote ( "Solver for compressible premixed/partially-premixed combustion with" " turbulence modelling." ); #include "postProcess.H" #include "setRootCaseLists.H" #include "createTime.H" #include "createDynamicFvMesh.H" #include "createControl.H" #include "readCombustionProperties.H" #include "readGravitationalAcceleration.H" #include "createFields.H" #include "createFieldRefs.H" #include "initContinuityErrs.H" #include "createRhoUf.H" #include "createControls.H" #include "initContinuityErrs.H" #include "compressibleCourantNo.H" #include "setInitialDeltaT.H" turbulence->validate(); // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // Info<< "\nStarting time loop\n" << endl; while (runTime.run()) { #include "createTimeControls.H" { // Store divrhoU from the previous mesh so that it can be mapped // and used in correctPhi to ensure the corrected phi has the // same divergence volScalarField divrhoU ( "divrhoU", fvc::div(fvc::absolute(phi, rho, U)) ); #include "compressibleCourantNo.H" #include "setDeltaT.H" ++runTime; Info<< "Time = " << runTime.timeName() << nl << endl; // Store momentum to set rhoUf for introduced faces. volVectorField rhoU("rhoU", rho*U); // Do any mesh changes mesh.update(); if (mesh.changing() && correctPhi) { // Calculate absolute flux from the mapped surface velocity phi = mesh.Sf() & rhoUf; #include "correctPhi.H" // Make the fluxes relative to the mesh-motion fvc::makeRelative(phi, rho, U); } } if (mesh.changing() && checkMeshCourantNo) { #include "meshCourantNo.H" } #include "rhoEqn.H" Info<< "rho min/max : " << min(rho).value() << " " << max(rho).value() << endl; // --- Pressure-velocity PIMPLE corrector loop while (pimple.loop()) { #include "UEqn.H" #include "ftEqn.H" #include "bEqn.H" #include "EauEqn.H" #include "EaEqn.H" if (!ign.ignited()) { thermo.heu() == thermo.he(); } // --- Pressure corrector loop while (pimple.correct()) { #include "pEqn.H" } if (pimple.turbCorr()) { turbulence->correct(); } } rho = thermo.rho(); runTime.write(); runTime.printExecutionTime(Info); } Info<< "End\n" << endl; return 0; } // ************************************************************************* //