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Author SHA1 Message Date
Henry
e20e69992d shallowWaterFoam: Read hU rather than U to support complex e.g. time-varying BCs 
Disadvantage is that the BC values have to be specified in terms of hU
rather than U.  The alternative would be to add complex code to map h
and U BCs into the equivalent for hU.
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1566
 2015-03-13 22:14:08 +00:00
Henry
de9ebcc299 Revert "Revert "Revert "DPMFoam: Multiply the gravitational force by the gas phase fraction""" 
This reverts commit c935f83ece.
 2015-03-13 14:39:01 +00:00
Henry
fd069939c1 rhoCentralFoam: Correct handling of single-cell meshes 
Resolves bug-report http://openfoam.org/mantisbt/view.php?id=1548
 2015-03-13 09:51:33 +00:00
Henry
43aec8425b TomiyamaLift: Updated coefficient to make the model continuous at EoH = 10.7 
Correction provided by Juho Peltola
 2015-03-11 18:06:04 +00:00
Henry
c935f83ece Revert "Revert "DPMFoam: Multiply the gravitational force by the gas phase fraction"" 
This reverts commit f5d26ab69b.
 2015-03-11 17:33:14 +00:00
Henry
f5d26ab69b Revert "DPMFoam: Multiply the gravitational force by the gas phase fraction" 
This reverts commit 49fbe73ac0.
 2015-03-11 15:47:29 +00:00
Henry
49fbe73ac0 DPMFoam: Multiply the gravitational force by the gas phase fraction 
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1563
 2015-03-11 10:50:32 +00:00
Henry
2e2cbe50c6 TomiyamaLift: Corrected coefficients to correspond exactly to the original paper cited 
Resolved bug-report http://www.openfoam.org/mantisbt/view.php?id=1564
 2015-03-10 19:57:42 +00:00
Henry
c239b0ebe0 Update Header 2015-03-02 22:30:29 +00:00
Henry
b82911b3cf BinghamPlastic: Change definition of shear-rate by 1/sqrt(2) 
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1552
 2015-03-02 22:27:39 +00:00
Henry
a12281827e Removed temporary Info 2015-03-02 22:26:24 +00:00
Henry
763ecdc0f4 rhoCentralFoam: Corrected the BCs for positive (outgoing) fluxes 
Resolves bug-report http://openfoam.org/mantisbt/view.php?id=1548
 2015-02-26 17:00:36 +00:00
Henry
0577cdb3cd rhoCentralDyMFoam: Add support for morphing-meshes and provide movingCone tutorial case 2015-02-25 12:20:12 +00:00
Henry
64ec856d60 rhoEqn: Do not constrain; would violate conservation 2015-02-22 16:50:48 +00:00
Henry
5daf22d9d7 interFoam/alphaEqn: Corrected handling of the off-centreing coefficient for Crank-Nicolson 2015-02-22 12:13:19 +00:00
Henry
ff8978dba5 interFoam/alphaEqn: Updated phiCN 2015-02-22 10:25:30 +00:00
Henry
9fc5f5c1db interFoam/alphaEqn: Update explicit corrector to use the Crank-Nicolson flux 2015-02-21 21:39:59 +00:00
Henry
5f24612805 icoFoam/nonNewtonianIcoFoam: Update to use pisoControl 2015-02-21 21:39:01 +00:00
Henry
47482b9246 LTSinterFoam: test for localEuler as a valid scheme in the new alphaEqn 2015-02-20 22:47:51 +00:00
Henry
218875bf40 DSMC: Rationalization and addition of mapping support 2015-02-20 17:24:14 +00:00
Henry
f78d33b634 interFoam family: Add support for MULES-bounded Crank-Nicolson 2nd-order ddt(alpha) 
This is an experimental feature demonstrating the potential of MULES to
create bounded solution which are 2nd-order in time AND space.

Crank-Nicolson may be selected on U and/or alpha but will only be fully
2nd-order if used on both within the PIMPLE-loop to converge the
interaction between the flux and phase-fraction.  Note also that
Crank-Nicolson may not be used with sub-cycling but all the features of
semi-implicit MULES are available in particular MULESCorr and
alphaApplyPrevCorr.

Examples of ddt specification:

ddtSchemes
{
    default         Euler;
}

ddtSchemes
{
    default         CrankNicolson 0.9;
}

ddtSchemes
{
    default         none;
    ddt(alpha)      CrankNicolson 0.9;
    ddt(rho,U)      CrankNicolson 0.9;
}

ddtSchemes
{
    default         none;
    ddt(alpha)      Euler;
    ddt(rho,U)      CrankNicolson 0.9;
}

ddtSchemes
{
    default         none;
    ddt(alpha)      CrankNicolson 0.9;
    ddt(rho,U)      Euler;
}

In these examples a small amount of off-centering in used to stabilize
the Crank-Nicolson scheme.  Also the specification for alpha1 is via the
generic phase-fraction name to ensure in multiphase solvers (when
Crank-Nicolson support is added) the scheme is identical for all phase
fractions.
 2015-02-20 15:59:43 +00:00
Henry
e593fef659 potentialFoam: Added new method to estimate the static pressure field from the velocity 
Uses a form of the Euler equation in which only variation along the streamlines is considered
 2015-02-19 19:05:17 +00:00
Henry
4db6925cee Thermodyamics: Add support for multiphase 
Pass the phase-name through hierarchy
Add phase-name to variables
Split basicCombustionMixture
Update applications accordingly
 2015-02-18 21:21:22 +00:00
Henry
f5c0684463 Updated header 2015-02-17 23:59:13 +00:00
Henry
e9f2981d85 driftFluxFoam: Updated base-class of incompressibleTwoPhaseInteractingMixture 2015-02-17 23:58:44 +00:00
Henry
76c7f68ac1 fluidThermo: Add compressibleTransportModel as base-class 
Needed to create generic compressible turbulence model library
 2015-02-17 17:25:26 +00:00
Henry
3429d2dd80 chtMultiRegionSimpleFoam: Support simpler input for rhoMax and rhoMin 2015-02-17 15:06:31 +00:00
Henry
c7f5b4ce17 applications/solvers: Update trans-sonic option in pEqns to by consistent with sonic-solvers 2015-02-17 10:47:34 +00:00
Henry
e8e0c99790 DyM solvers: rationalized handling of time update 2015-02-16 21:48:00 +00:00
Henry
74990ee915 Rationalized sprayFoam family of solvers and added sprayDyMFoam 2015-02-16 21:47:15 +00:00
Henry
5a9fc9a3e9 Rationalized pEqn in sprayFoam solvers 2015-02-16 21:45:28 +00:00
Henry
cec56de03e Compressible solvers: rhoMax and rhoMin now optional and may be supplied without dimensions 2015-02-16 21:43:40 +00:00
Henry
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
Henry
f58fd14271 Corrected capitalization of Doxygen documentation comments 2015-02-14 13:10:15 +00:00
Henry
cdadf4865d potentialFoam: Solve for velocity potential named Phi rather than using the pressure field for this purpose 
The Phi field is read if available otherwise created automatically with
boundary conditions obtained automatically from the pressure field if
available (with optional name) otherwise inferred from the velocity
field.  Phi Laplacian scheme and solver specification are required.  See
tutorials for examples.
 2015-02-14 11:03:37 +00:00
Henry
aee9511710 porousInterFoam is no longer needed 
Use interFoam with fvOptions
 2015-02-13 21:39:48 +00:00
Henry
e13210a6d6 twoPhaseEulerFoam/twoPhaseSystem/diameterModels/IATE: Corrected sign of random coalescence source 
Resolves bug-report http://openfoam.org/mantisbt/view.php?id=1382
 2015-02-13 09:23:22 +00:00
Henry
e636b7c73b Correct section comment: there can only be one destructor 2015-02-12 21:57:29 +00:00
Henry
d6ca208a50 rhoCentralDyMFoam: Name intermediate fields to avoid duplicate registration 
Updated mesh-motion functionality
 2015-02-12 13:17:28 +00:00
Henry
7d3f1067c7 Update headers 2015-02-12 12:34:27 +00:00
Henry
018de2e37a Name fields to avoid duplicate registration 2015-02-12 12:33:45 +00:00
Henry
a4f46eb5e6 pEqn: DO NOT constrain the pressure equation as this will lead to continuity errors 2015-02-12 10:42:17 +00:00
Henry
a4cca549e2 Explicitly name derived fields to improve readability of diagnostic messages and avoid duplicate registration 2015-02-12 09:59:52 +00:00
Henry
92e0c46ad1 kineticTheoryModel: Name intermediate variable and avoid duplicate registration 2015-02-11 16:51:44 +00:00
Henry
5a896b95df driftFluxFoam: Name ghf correctly 
Avoids problem of duplicate registration
 2015-02-11 14:49:23 +00:00
Henry
bdd5c4b8d3 twoPhaseEulerFoam/twoPhaseSystem/diameterModels/constantDiameter: Do not register the temporary diameter field 2015-02-11 14:48:34 +00:00
Henry
e939d1de79 Solvers: Rationalized correctPhi 2015-02-11 13:22:24 +00:00
Henry
def52a306a Formatting: Rationalized the indentation of #include 2015-02-10 20:35:50 +00:00
Henry
4a3dce9e8f solvers: rationalize the construction of the fvOptions 2015-02-10 18:33:45 +00:00
Henry
1b56ed238b solvers: rationalize the return statement 2015-02-10 18:20:42 +00:00