Files
OpenFOAM-12/applications/solvers/combustion/PDRFoam/PDRFoamAutoRefine.C
Henry Weller cf3d6cd1e9 fvMeshMovers, fvMeshTopoChangers: General mesh motion and topology change replacement for dynamicFvMesh
Mesh motion and topology change are now combinable run-time selectable options
within fvMesh, replacing the restrictive dynamicFvMesh which supported only
motion OR topology change.

All solvers which instantiated a dynamicFvMesh now instantiate an fvMesh which
reads the optional constant/dynamicFvMeshDict to construct an fvMeshMover and/or
an fvMeshTopoChanger.  These two are specified within the optional mover and
topoChanger sub-dictionaries of dynamicFvMeshDict.

When the fvMesh is updated the fvMeshTopoChanger is first executed which can
change the mesh topology in anyway, adding or removing points as required, for
example for automatic mesh refinement/unrefinement, and all registered fields
are mapped onto the updated mesh.  The fvMeshMover is then executed which moved
the points only and calculates the cell volume change and corresponding
mesh-fluxes for conservative moving mesh transport.  If multiple topological
changes or movements are required these would be combined into special
fvMeshMovers and fvMeshTopoChangers which handle the processing of a list of
changes, e.g. solidBodyMotionFunctions:multiMotion.

The tutorials/multiphase/interFoam/laminar/sloshingTank3D3DoF case has been
updated to demonstrate this new functionality by combining solid-body motion
with mesh refinement/unrefinement:

/*--------------------------------*- C++ -*----------------------------------*\
  =========                 |
  \\      /  F ield         | OpenFOAM: The Open Source CFD Toolbox
   \\    /   O peration     | Website:  https://openfoam.org
    \\  /    A nd           | Version:  dev
     \\/     M anipulation  |
\*---------------------------------------------------------------------------*/
FoamFile
{
    format      ascii;
    class       dictionary;
    location    "constant";
    object      dynamicMeshDict;
}
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //

mover
{
    type    motionSolver;

    libs    ("libfvMeshMovers.so" "libfvMotionSolvers.so");

    motionSolver    solidBody;

    solidBodyMotionFunction SDA;

    CofG            (0 0 0);
    lamda           50;
    rollAmax        0.2;
    rollAmin        0.1;
    heaveA          4;
    swayA           2.4;
    Q               2;
    Tp              14;
    Tpn             12;
    dTi             0.06;
    dTp             -0.001;
}

topoChanger
{
    type    refiner;

    libs    ("libfvMeshTopoChangers.so");

    // How often to refine
    refineInterval  1;

    // Field to be refinement on
    field           alpha.water;

    // Refine field in between lower..upper
    lowerRefineLevel 0.001;
    upperRefineLevel 0.999;

    // Have slower than 2:1 refinement
    nBufferLayers   1;

    // Refine cells only up to maxRefinement levels
    maxRefinement   1;

    // Stop refinement if maxCells reached
    maxCells        200000;

    // Flux field and corresponding velocity field. Fluxes on changed
    // faces get recalculated by interpolating the velocity. Use 'none'
    // on surfaceScalarFields that do not need to be reinterpolated.
    correctFluxes
    (
        (phi none)
        (nHatf none)
        (rhoPhi none)
        (alphaPhi.water none)
        (meshPhi none)
        (meshPhi_0 none)
        (ghf none)
    );

    // Write the refinement level as a volScalarField
    dumpLevel       true;
}

// ************************************************************************* //

Note that currently this is the only working combination of mesh-motion with
topology change within the new framework and further development is required to
update the set of topology changers so that topology changes with mapping are
separated from the mesh-motion so that they can be combined with any of the
other movements or topology changes in any manner.

All of the solvers and tutorials have been updated to use the new form of
dynamicMeshDict but backward-compatibility was not practical due to the complete
reorganisation of the mesh change structure.
2021-10-01 15:50:06 +01:00

216 lines
6.6 KiB
C++

/*---------------------------------------------------------------------------*\
========= |
\\ / F ield | OpenFOAM: The Open Source CFD Toolbox
\\ / O peration | Website: https://openfoam.org
\\ / A nd | Copyright (C) 2011-2021 OpenFOAM Foundation
\\/ 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 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
PDRFoam
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 incorporated 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 "psiuReactionThermo.H"
#include "compressibleMomentumTransportModels.H"
#include "fluidThermophysicalTransportModel.H"
#include "laminarFlameSpeed.H"
#include "XiModel.H"
#include "PDRDragModel.H"
#include "ignition.H"
#include "Switch.H"
#include "bound.H"
#include "pimpleControl.H"
#include "fvModels.H"
#include "fvConstraints.H"
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
int main(int argc, char *argv[])
{
#include "postProcess.H"
#include "setRootCaseLists.H"
#include "createTime.H"
#include "createMesh.H"
#include "createControl.H"
#include "readCombustionProperties.H"
#include "readGravitationalAcceleration.H"
#include "createFields.H"
#include "createFieldRefs.H"
#include "initContinuityErrs.H"
#include "createTimeControls.H"
#include "compressibleCourantNo.H"
#include "setInitialDeltaT.H"
turbulence->validate();
scalar StCoNum = 0.0;
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
Info<< "\nStarting time loop\n" << endl;
bool hasChanged = false;
while (pimple.run(runTime))
{
#include "readTimeControls.H"
#include "compressibleCourantNo.H"
#include "setDeltaT.H"
// Indicators for refinement. Note: before runTime++
// only for postprocessing reasons.
tmp<volScalarField> tmagGradP = mag(fvc::grad(p));
volScalarField normalisedGradP
(
"normalisedGradP",
tmagGradP()/max(tmagGradP())
);
normalisedGradP.writeOpt() = IOobject::AUTO_WRITE;
tmagGradP.clear();
runTime++;
Info<< "\n\nTime = " << runTime.timeName() << endl;
{
// Make the fluxes absolute
fvc::makeAbsolute(phi, rho, U);
// Test : disable refinement for some cells
// PackedBoolList& protectedCell =
// refCast<dynamicRefineFvMesh>(mesh).protectedCell();
// if (protectedCell.empty())
// {
// protectedCell.setSize(mesh.nCells());
// protectedCell = 0;
// }
// forAll(betav, celli)
// {
// if (betav[celli] < 0.99)
// {
// protectedCell[celli] = 1;
// }
// }
// Flux estimate for introduced faces.
volVectorField rhoU("rhoU", rho*U);
// Do any mesh changes
bool meshChanged = mesh.update();
if (meshChanged)
{
hasChanged = true;
}
if (runTime.write() && hasChanged)
{
betav.write();
Lobs.write();
CT.write();
drag->writeFields();
flameWrinkling->writeFields();
hasChanged = false;
}
// Make the fluxes relative to the mesh motion
fvc::makeRelative(phi, rho, U);
}
#include "rhoEqn.H"
// --- Pressure-velocity PIMPLE corrector loop
while (pimple.loop())
{
fvModels.correct();
#include "UEqn.H"
// --- Pressure corrector loop
while (pimple.correct())
{
#include "bEqn.H"
#include "ftEqn.H"
#include "EauEqn.H"
#include "EaEqn.H"
if (!ign.ignited())
{
thermo.heu() == thermo.he();
}
#include "pEqn.H"
}
if (pimple.turbCorr())
{
turbulence->correct();
thermophysicalTransport->correct();
}
}
runTime.write();
Info<< "\nExecutionTime = "
<< runTime.elapsedCpuTime()
<< " s\n" << endl;
}
Info<< "\n end\n";
return 0;
}
// ************************************************************************* //