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foam-extend4.1-coherent-io/applications/solvers/combustion/engineFoam/engineFoam.C
2015-05-17 15:58:16 +02:00

133 lines
4.1 KiB
C

/*---------------------------------------------------------------------------*\
========= |
\\ / F ield | foam-extend: Open Source CFD
\\ / O peration | Version: 3.2
\\ / A nd | Web: http://www.foam-extend.org
\\/ M anipulation | For copyright notice see file Copyright
-------------------------------------------------------------------------------
License
This file is part of foam-extend.
foam-extend 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.
foam-extend 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 foam-extend. If not, see <http://www.gnu.org/licenses/>.
Application
engineFoam
Description
Solver for internal combustion engines.
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.
\*---------------------------------------------------------------------------*/
#include "fvCFD.H"
#include "engineTime.H"
#include "engineMesh.H"
#include "hhuCombustionThermo.H"
#include "turbulenceModel.H"
#include "laminarFlameSpeed.H"
#include "ignition.H"
#include "Switch.H"
#include "OFstream.H"
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
int main(int argc, char *argv[])
{
# include "setRootCase.H"
# include "createEngineTime.H"
# include "createEngineMesh.H"
# include "readCombustionProperties.H"
# include "createFields.H"
# include "initContinuityErrs.H"
# include "readEngineTimeControls.H"
# include "compressibleCourantNo.H"
# include "setInitialDeltaT.H"
# include "startSummary.H"
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
Info << "\nStarting time loop\n" << endl;
while (runTime.run())
{
# include "readPISOControls.H"
# include "readEngineTimeControls.H"
# include "compressibleCourantNo.H"
# include "setDeltaT.H"
runTime++;
Info<< "Crank angle = " << runTime.theta() << " CA-deg" << endl;
mesh.move();
# include "rhoEqn.H"
# include "UEqn.H"
// --- PISO loop
for (int corr=1; corr<=nCorr; corr++)
{
# include "ftEqn.H"
# include "bEqn.H"
# include "huEqn.H"
# include "hEqn.H"
if (!ign.ignited())
{
hu == h;
}
# include "pEqn.H"
}
turbulence->correct();
# include "logSummary.H"
rho = thermo.rho();
runTime.write();
Info<< "ExecutionTime = " << runTime.elapsedCpuTime() << " s"
<< " ClockTime = " << runTime.elapsedClockTime() << " s"
<< nl << endl;
}
Info<< "End\n" << endl;
return 0;
}
// ************************************************************************* //