Reduce the number of phaseSystems libraries:
- phaseSystems previously had a number of smaller libraries to provide
interface and model properties, etc. This potential flexibility was
never actually used anywhere, but causes cyclic dependencies between
phaseSystem and the models (and turbulence) that causes extreme
difficulty for mingw linking (issue #1238).
- libincompressibleMultiphaseSystems
- removed: libmassTransferModels
- libmultiphaseSystem
- removed: libcompressibleMultiphaseEulerianInterfacialModels
- libreactingMultiphaseSystem
- removed: libreactingPhaseSystem
- removed: libreactingEulerianFvPatchFields
- removed: libreactingEulerianInterfacialCompositionModels
- removed: libreactingEulerianInterfacialModels
- removed: libmultiphaseReactingTurbulenceModels
- libreactingTwoPhaseSystem
- removed: libreactingPhaseSystem
- removed: libreactingEulerianFvPatchFields
- removed: libreactingEulerianInterfacialCompositionModels
- removed: libreactingEulerianInterfacialModels
Avoid duplicate symbol for phaseCompressibleTurbulenceModels
Common turbulence models are defined in libreactingMultiphaseSystem,
and libmultiphaseReactingTurbulenceModels is now redundant.
The libtwoPhaseReactingTurbulenceModels extends the common models
for reactingTwoPhaseSystem.
The interfacial temperature is assumed equal to the saturation
temperature. Only a single species is considered volatile and the other
species to not affect the mass-transfer.
Currently this is implemented only for the Antoine equation, for the
other more complex models an iterative inversion from pressure to
temperature is required.
Select LTS via the ddtScheme:
ddtSchemes
{
default localEuler rDeltaT;
}
The LTS algorithm is currently controlled with the standard settings in
controlDict, e.g.:
maxCo 0.5;
maxDeltaT 2e-8;
with the addition of the optional rDeltaT smoothing coefficient:
rDeltaTSmoothingCoeff 0.02;
which defaults to 0.02.
ddtSchemes
{
default localEuler rDeltaT;
}
Multi-species, mass-transfer and reaction support and multi-phase
structure provided by William Bainbridge.
Integration of the latest p-U and face-p_U algorithms with William's
multi-phase structure is not quite complete due to design
incompatibilities which needs further development. However the
integration of the functionality is complete.
The results of the tutorials are not exactly the same for the
twoPhaseEulerFoam and reactingTwoPhaseEulerFoam solvers but are very
similar. Further analysis in needed to ensure these differences are
physical or to resolve them; in the meantime the twoPhaseEulerFoam
solver will be maintained.
