Commit Graph

12 Commits

Author SHA1 Message Date
13d4f5c386 Buoyant solvers: Add special handling for ghRef in the case g = (0 0 0) 2015-03-19 15:26:06 +00:00
afcd290d75 Solvers based on p_rgh: Added support for optional hRef
Allows the specification of a reference height, for example the height
of the free-surface in a VoF simulation, which reduces the range of p_rgh.

hRef is a uniformDimensionedScalarField specified via the constant/hRef
file, equivalent to the way in which g is specified, so that it can be
looked-up from the database.  For example see the constant/hRef file in
the DTCHull LTSInterFoam and interDyMFoam cases.
2015-03-17 17:15:11 +00:00
cd5ade6c44 compressibleInterDyMFoam and interPhaseChangeDyMFoam: cache divU before time advancement to ensure the old-time meshPhi are used to make phi absolute
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1531
2015-02-16 21:42:09 +00:00
f58fd14271 Corrected capitalization of Doxygen documentation comments 2015-02-14 13:10:15 +00:00
a4cca549e2 Explicitly name derived fields to improve readability of diagnostic messages and avoid duplicate registration 2015-02-12 09:59:52 +00:00
e939d1de79 Solvers: Rationalized correctPhi 2015-02-11 13:22:24 +00:00
4a3dce9e8f solvers: rationalize the construction of the fvOptions 2015-02-10 18:33:45 +00:00
927498accb Applications: use pimpleControl.dict() and simpleControl.dict() instead of looking-up the sub-dict 2015-02-09 22:15:26 +00:00
9053fefa6c multiphase solvers: print phase-name rather than alpha1/2 when printing max and min phase-fraction 2015-01-21 20:07:15 +00:00
93732c8af4 Updated the whole of OpenFOAM to use the new templated TurbulenceModels library
The old separate incompressible and compressible libraries have been removed.

Most of the commonly used RANS and LES models have been upgraded to the
new framework but there are a few missing which will be added over the
next few days, in particular the realizable k-epsilon model.  Some of
the less common incompressible RANS models have been introduced into the
new library instantiated for incompressible flow only.  If they prove to
be generally useful they can be templated for compressible and
multiphase application.

The Spalart-Allmaras DDES and IDDES models have been thoroughly
debugged, removing serious errors concerning the use of S rather than
Omega.

The compressible instances of the models have been augmented by a simple
backward-compatible eddyDiffusivity model for thermal transport based on
alphat and alphaEff.  This will be replaced with a separate run-time
selectable thermal transport model framework in a few weeks.

For simplicity and ease of maintenance and further development the
turbulent transport and wall modeling is based on nut/nuEff rather than
mut/muEff for compressible models so that all forms of turbulence models
can use the same wall-functions and other BCs.

All turbulence model selection made in the constant/turbulenceProperties
dictionary with RAS and LES as sub-dictionaries rather than in separate
files which added huge complexity for multiphase.

All tutorials have been updated so study the changes and update your own
cases by comparison with similar cases provided.

Sorry for the inconvenience in the break in backward-compatibility but
this update to the turbulence modeling is an essential step in the
future of OpenFOAM to allow more models to be added and maintained for a
wider range of cases and physics.  Over the next weeks and months more
turbulence models will be added of single and multiphase flow, more
additional sub-models and further development and testing of existing
models.  I hope this brings benefits to all OpenFOAM users.

Henry G. Weller
2015-01-21 19:21:39 +00:00
bc5134a55e New version of wmake supporting out-of-tree object and dependency files 2014-12-14 21:42:18 +00:00
446e5777f0 Add the OpenFOAM source tree 2014-12-10 22:40:10 +00:00