Commit ea17556c authored by shunbo's avatar shunbo
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/*---------------------------------------------------------------------------*\
========= |
\\ / F ield | OpenFOAM: The Open Source CFD Toolbox
\\ / O peration |
\\ / A nd | www.openfoam.com
\\/ M anipulation |
-------------------------------------------------------------------------------
Copyright (C) 2011-2012 OpenFOAM Foundation
-------------------------------------------------------------------------------
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 <http://www.gnu.org/licenses/>.
Class
Foam::laminarFlameSpeedModels::SCOPE
Description
Laminar flame speed obtained from the SCOPE correlation.
Seven parameters are specified in terms of polynomial functions of
stoichiometry. Two polynomials are fitted, covering different parts of the
flammable range. If the mixture is outside the fitted range, linear
interpolation is used between the extreme of the polynomio and the upper or
lower flammable limit with the Markstein number constant.
Variations of pressure and temperature from the reference values are taken
into account through \f$ pexp \f$ and \f$ texp \f$
The laminar burning velocity fitting polynomial is:
\f$ Su = a_{0}(1+a_{1}x+K+..a_{i}x^{i}..+a_{6}x^{6}) (p/p_{ref})^{pexp}
(T/T_{ref})^{texp} \f$
where:
\f$ a_{i} \f$ are the polinomial coefficients.
\f$ pexp \f$ and \f$ texp \f$ are the pressure and temperature factors
respectively.
\f$ x \f$ is the equivalence ratio.
\f$ T_{ref} \f$ and \f$ p_{ref} \f$ are the temperature and pressure
references for the laminar burning velocity.
SourceFiles
SCOPELaminarFlameSpeed.C
\*---------------------------------------------------------------------------*/
#ifndef SCOPE_H
#define SCOPE_H
#include "laminarFlameSpeed.H"
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
namespace Foam
{
namespace laminarFlameSpeedModels
{
/*---------------------------------------------------------------------------*\
Class SCOPE Declaration
\*---------------------------------------------------------------------------*/
class SCOPE
:
public laminarFlameSpeed
{
// Private Data
class polynomial
:
public FixedList<scalar, 7>
{
public:
//- Lower limit
scalar ll;
//- Upper polynomial limit
scalar ul;
//- Value at lower limit
scalar llv;
//- Value at upper limit
scalar ulv;
//- Changeover point from lower to upper polynomial
scalar lu;
//- Construct from dictionary
polynomial(const dictionary& polyDict);
};
dictionary coeffsDict_;
//- Lower flammability limit
scalar LFL_;
//- Upper flammability limit
scalar UFL_;
//- Lower Su polynomial
polynomial SuPolyL_;
//- Upper Su polynomial
polynomial SuPolyU_;
//- Temperature correction exponent
scalar Texp_;
//- Pressure correction exponent
scalar pexp_;
//- Lower Ma polynomial
polynomial MaPolyL_;
//- Upper Ma polynomial
polynomial MaPolyU_;
// Private member functions
//- Polynomial evaluated from the given equivalence ratio
// and polynomial coefficients
static inline scalar polyPhi(scalar phi, const polynomial& a);
//- Laminar flame speed evaluated from the given equivalence ratio
// at the reference temperature and pressure
inline scalar SuRef(scalar phi) const;
//- Markstein evaluated from the given equivalence ratio
inline scalar Ma(scalar phi) const;
//- Laminar flame speed evaluated from the given equivalence ratio
// corrected for temperature and pressure dependence
inline scalar Su0pTphi(scalar p, scalar Tu, scalar phi) const;
//- Laminar flame speed evaluated from the given uniform
// equivalence ratio corrected for temperature and pressure dependence
tmp<volScalarField> Su0pTphi
(
const volScalarField& p,
const volScalarField& Tu,
scalar phi
) const;
//- Laminar flame speed evaluated from the given equivalence ratio
// distribution corrected for temperature and pressure dependence
tmp<volScalarField> Su0pTphi
(
const volScalarField& p,
const volScalarField& Tu,
const volScalarField& phi
) const;
//- Return the Markstein number
// evaluated from the given equivalence ratio
tmp<volScalarField> Ma(const volScalarField& phi) const;
//- Construct as copy (not implemented)
SCOPE(const SCOPE&);
void operator=(const SCOPE&);
public:
//- Runtime type information
TypeName("SCOPE");
// Constructors
//- Construct from dictionary and psiuReactionThermo
SCOPE
(
const dictionary&,
const psiuReactionThermo&
);
//- Destructor
~SCOPE();
// Member functions
//- Return the Markstein number
tmp<volScalarField> Ma() const;
//- Return the laminar flame speed [m/s]
tmp<volScalarField> operator()() const;
};
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
} // End laminarFlameSpeedModels
} // End namespace Foam
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
#endif
// ************************************************************************* //
rho = thermo.rho();
volScalarField rAU(1.0/UEqn.A());
volVectorField HbyA(constrainHbyA(invA & UEqn.H(), U, p));
if (pimple.transonic())
{
surfaceScalarField phid
(
"phid",
fvc::interpolate(psi)
*(
fvc::flux(HbyA)
+ fvc::interpolate(rho*rAU)*fvc::ddtCorr(rho, U, phi)
/fvc::interpolate(rho)
)
);
while (pimple.correctNonOrthogonal())
{
fvScalarMatrix pEqn
(
betav*fvm::ddt(psi, p)
+ fvm::div(phid, p)
- fvm::laplacian(rho*invA, p)
==
betav*fvOptions(psi, p, rho.name())
);
pEqn.solve(mesh.solver(p.select(pimple.finalInnerIter())));
if (pimple.finalNonOrthogonalIter())
{
phi == pEqn.flux();
}
}
}
else
{
surfaceScalarField phiHbyA
(
"phiHbyA",
(
fvc::flux(rho*HbyA)
+ fvc::interpolate(rho*rAU)*fvc::ddtCorr(rho, U, phi)
)
);
while (pimple.correctNonOrthogonal())
{
fvScalarMatrix pEqn
(
betav*fvm::ddt(psi, p)
+ fvc::div(phiHbyA)
- fvm::laplacian(rho*invA, p)
==
betav*fvOptions(psi, p, rho.name())
);
pEqn.solve(mesh.solver(p.select(pimple.finalInnerIter())));
if (pimple.finalNonOrthogonalIter())
{
phi = phiHbyA + pEqn.flux();
}
}
}
#include "rhoEqn.H"
#include "continuityErrs.H"
U = HbyA - (invA & (betav*fvc::grad(p)));
U.correctBoundaryConditions();
fvOptions.correct(U);
K = 0.5*magSqr(U);
if (thermo.dpdt())
{
dpdt = fvc::ddt(p);
}
Info<< "Reading combustion properties\n" << endl;
IOdictionary combustionProperties
(
IOobject
(
"combustionProperties",
runTime.constant(),
mesh,
IOobject::MUST_READ_IF_MODIFIED,
IOobject::NO_WRITE
)
);
ignition ign(combustionProperties, runTime, mesh);
/*---------------------------------------------------------------------------*\
========= |
\\ / F ield | OpenFOAM: The Open Source CFD Toolbox
\\ / O peration |
\\ / A nd | www.openfoam.com
\\/ M anipulation |
-------------------------------------------------------------------------------
Copyright (C) 2011 OpenFOAM Foundation
-------------------------------------------------------------------------------
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 <http://www.gnu.org/licenses/>.
Global
rhoEqn
Description
Solve the continuity for density.
\*---------------------------------------------------------------------------*/
{
solve(betav*fvm::ddt(rho) + fvc::div(phi));
}
// ************************************************************************* //
/*---------------------------------------------------------------------------*\
========= |
\\ / F ield | OpenFOAM: The Open Source CFD Toolbox
\\ / O peration |
\\ / A nd | www.openfoam.com
\\/ M anipulation |
-------------------------------------------------------------------------------
Copyright (C) 2011 OpenFOAM Foundation
-------------------------------------------------------------------------------
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 <http://www.gnu.org/licenses/>.
Global
setDeltaT
Description
Reset the timestep to maintain a constant maximum courant Number.
Reduction of time-step is immediate but increase is damped to avoid
unstable oscillations.
\*---------------------------------------------------------------------------*/
if (adjustTimeStep)
{
scalar maxDeltaTFact = maxCo/(CoNum + StCoNum + SMALL);
scalar deltaTFact = min(min(maxDeltaTFact, 1.0 + 0.1*maxDeltaTFact), 1.2);
runTime.setDeltaT
(
min
(
deltaTFact*runTime.deltaTValue(),
maxDeltaT
)
);
Info<< "deltaT = " << runTime.deltaTValue() << endl;
}
// ************************************************************************* //
{
volScalarField& hea = thermo.he();
fvScalarMatrix EaEqn
(
fvm::ddt(rho, hea) + mvConvection->fvmDiv(phi, hea)
+ fvc::ddt(rho, K) + fvc::div(phi, K)
+ (
hea.name() == "ea"
? fvc::div
(
fvc::absolute(phi/fvc::interpolate(rho), U),
p,
"div(phiv,p)"
)
: -dpdt
)
- fvm::laplacian(turbulence->alphaEff(), hea)
+ fvOptions(rho, hea)
);
EaEqn.relax();
fvOptions.constrain(EaEqn);
EaEqn.solve();
fvOptions.correct(hea);
thermo.correct();
}
if (ign.ignited())
{
volScalarField& heau = thermo.heu();
fvScalarMatrix heauEqn
(
fvm::ddt(rho, heau) + mvConvection->fvmDiv(phi, heau)
+ (fvc::ddt(rho, K) + fvc::div(phi, K))*rho/thermo.rhou()
+ (
heau.name() == "eau"
? fvc::div
(
fvc::absolute(phi/fvc::interpolate(rho), U),
p,
"div(phiv,p)"
)*rho/thermo.rhou()
: -dpdt*rho/thermo.rhou()
)
- fvm::laplacian(turbulence->alphaEff(), heau)
// These terms cannot be used in partially-premixed combustion due to
// the resultant inconsistency between ft and heau transport.
// A possible solution would be to solve for ftu as well as ft.
//- fvm::div(muEff*fvc::grad(b)/(b + 0.001), heau)
//+ fvm::Sp(fvc::div(muEff*fvc::grad(b)/(b + 0.001)), heau)
==
fvOptions(rho, heau)
);
fvOptions.constrain(heauEqn);
heauEqn.solve();
fvOptions.correct(heau);
}
XiFoam.C
EXE = $(FOAM_APPBIN)/XiFoam
EXE_INC = \
-I$(LIB_SRC)/finiteVolume/lnInclude \
-I$(LIB_SRC)/meshTools/lnInclude \
-I$(LIB_SRC)/sampling/lnInclude \
-I$(LIB_SRC)/engine/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/specie/lnInclude \
-I$(LIB_SRC)/transportModels/compressible/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/basic/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/reactionThermo/lnInclude \
-I$(LIB_SRC)/TurbulenceModels/turbulenceModels/lnInclude \
-I$(LIB_SRC)/TurbulenceModels/compressible/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/laminarFlameSpeed/lnInclude
EXE_LIBS = \
-lfiniteVolume \
-lfvOptions \
-lmeshTools \
-lsampling \
-lengine \
-lturbulenceModels \
-lcompressibleTurbulenceModels \
-lcompressibleTransportModels \
-lfluidThermophysicalModels \
-lreactionThermophysicalModels \
-lspecie \
-llaminarFlameSpeedModels
MRF.correctBoundaryVelocity(U);
fvVectorMatrix UEqn
(
fvm::ddt(rho, U) + fvm::div(phi, U)
+ MRF.DDt(rho, U)
+ turbulence->divDevRhoReff(U)
==
fvOptions(rho, U)
);
UEqn.relax();
fvOptions.constrain(UEqn);
if (pimple.momentumPredictor())
{
solve(UEqn == -fvc::grad(p));
fvOptions.correct(U);
K = 0.5*magSqr(U);
}
XiDyMFoam.C
EXE = $(FOAM_APPBIN)/XiDyMFoam
EXE_INC = \
-I.. \
-I$(LIB_SRC)/finiteVolume/lnInclude \
-I$(LIB_SRC)/fvOptions/lnInclude \
-I$(LIB_SRC)/meshTools/lnInclude \
-I$(LIB_SRC)/dynamicMesh/lnInclude \
-I$(LIB_SRC)/dynamicFvMesh/lnInclude \
-I$(LIB_SRC)/sampling/lnInclude \
-I$(LIB_SRC)/engine/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/specie/lnInclude \
-I$(LIB_SRC)/transportModels/compressible/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/basic/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/reactionThermo/lnInclude \
-I$(LIB_SRC)/TurbulenceModels/turbulenceModels/lnInclude \
-I$(LIB_SRC)/TurbulenceModels/compressible/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/laminarFlameSpeed/lnInclude
EXE_LIBS = \
-lfiniteVolume \
-lfvOptions \
-lmeshTools \
-ldynamicMesh \
-ldynamicFvMesh \
-ltopoChangerFvMesh \
-lsampling \
-lengine \
-lturbulenceModels \
-lcompressibleTurbulenceModels \
-lcompressibleTransportModels \
-lfluidThermophysicalModels \
-lreactionThermophysicalModels \
-lspecie \
-llaminarFlameSpeedModels
/*---------------------------------------------------------------------------*\
========= |
\\ / 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 <http://www.gnu.org/licenses/>.
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;
}
// ************************************************************************* //
CorrectPhi
(
U,
phi,
p,
rho,
psi,
dimensionedScalar("rAUf", dimTime, 1),
divrhoU,
pimple
);
#include "createTimeControls.H"
bool correctPhi
(
pimple.dict().getOrDefault("correctPhi", true)
);
bool checkMeshCourantNo
(
pimple.dict().getOrDefault("checkMeshCourantNo", false)
);
rho = thermo.rho();
volScalarField rAU(1.0/UEqn.A());
surfaceScalarField rhorAUf("rhorAUf", fvc::interpolate(rho*rAU));
volVectorField HbyA(constrainHbyA(rAU*UEqn.H(), U, p));
if (pimple.transonic())
{
surfaceScalarField phid
(
"phid",
fvc::interpolate(psi)
*(
(fvc::interpolate(HbyA) & mesh.Sf())
+ rhorAUf*fvc::ddtCorr(rho, U, phi)/fvc::interpolate(rho)
)
);
fvc::makeRelative(phid, psi, U);
MRF.makeRelative(fvc::interpolate(psi), phid);
while (pimple.correctNonOrthogonal())
{
fvScalarMatrix pEqn
(
fvm::ddt(psi, p)
+ fvm::div(phid, p)
- fvm::laplacian(rhorAUf, p)
==
fvOptions(psi, p, rho.name())
);
pEqn.solve(mesh.solver(p.select(pimple.finalInnerIter())));
if (pimple.finalNonOrthogonalIter())
{
phi == pEqn.flux();
}
}
}
else
{
surfaceScalarField phiHbyA
(
"phiHbyA",
(
(fvc::interpolate(rho*HbyA) & mesh.Sf())
+ rhorAUf*fvc::ddtCorr(rho, U, rhoUf)
)
);
fvc::makeRelative(phiHbyA, rho, U);
MRF.makeRelative(phiHbyA);
// Update the pressure BCs to ensure flux consistency
constrainPressure(p, rho, U, phiHbyA, rhorAUf, MRF);
while (pimple.correctNonOrthogonal())
{
fvScalarMatrix pEqn
(
fvm::ddt(psi, p)
+ fvc::div(phiHbyA)
- fvm::laplacian(rhorAUf, p)
==
fvOptions(psi, p, rho.name())
);
pEqn.solve(mesh.solver(p.select(pimple.finalInnerIter())));
if (pimple.finalNonOrthogonalIter())
{
phi = phiHbyA + pEqn.flux();
}
}
}
#include "rhoEqn.H"
#include "compressibleContinuityErrs.H"
U = HbyA - rAU*fvc::grad(p);
U.correctBoundaryConditions();
fvOptions.correct(U);
K = 0.5*magSqr(U);
{
rhoUf = fvc::interpolate(rho*U);
surfaceVectorField n(mesh.Sf()/mesh.magSf());
rhoUf += n*(fvc::absolute(phi, rho, U)/mesh.magSf() - (n & rhoUf));
}
if (thermo.dpdt())
{
dpdt = fvc::ddt(p);
if (mesh.moving())
{
dpdt -= fvc::div(fvc::meshPhi(rho, U), p);
}
}
#include "readTimeControls.H"
correctPhi = pimple.dict().getOrDefault("correctPhi", true);
checkMeshCourantNo =
pimple.dict().getOrDefault("checkMeshCourantNo", false);
XiEngineFoam.C
EXE = $(FOAM_APPBIN)/XiEngineFoam
EXE_INC = \
-I.. \
-I$(LIB_SRC)/finiteVolume/lnInclude \
-I$(LIB_SRC)/meshTools/lnInclude \
-I$(LIB_SRC)/sampling/lnInclude \
-I$(LIB_SRC)/engine/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/specie/lnInclude \
-I$(LIB_SRC)/transportModels/compressible/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/basic/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/reactionThermo/lnInclude \
-I$(LIB_SRC)/TurbulenceModels/turbulenceModels/lnInclude \
-I$(LIB_SRC)/TurbulenceModels/compressible/lnInclude \
-I$(LIB_SRC)/thermophysicalModels/laminarFlameSpeed/lnInclude
EXE_LIBS = \
-lfiniteVolume \
-lfvOptions \
-lmeshTools \
-lsampling \
-lengine \
-lturbulenceModels \
-lcompressibleTurbulenceModels \
-lcompressibleTransportModels \
-lfluidThermophysicalModels \
-lreactionThermophysicalModels \
-lspecie \
-llaminarFlameSpeedModels
fvVectorMatrix UEqn
(
fvm::ddt(rho, U)
+ fvm::div(phi, U)
+ turbulence->divDevRhoReff(U)
==
fvOptions(rho, U)
);
if (pimple.momentumPredictor())
{
solve(UEqn == -fvc::grad(p));
fvOptions.correct(U);
K = 0.5*magSqr(U);
}
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