Commit Graph

227 Commits

Author SHA1 Message Date
Chris Greenshields
344f435f54 Tutorials fvSolution files: removed solver entries which use default
values; formatted Switch entries consistently across all cases
2016-06-15 07:39:12 +01:00
Chris Greenshields
3d810c11dc Tutorials: made laplacianSchemes consistent and correct 2016-06-13 23:38:03 +01:00
Henry Weller
e4dc50dcb0 postProcessing: Replaced 'foamCalc' and the 'postCalc' utilities
with the more general and flexible 'postProcess' utility and '-postProcess' solver option

Rationale
---------

Both the 'postProcess' utility and '-postProcess' solver option use the
same extensive set of functionObjects available for data-processing
during the run avoiding the substantial code duplication necessary for
the 'foamCalc' and 'postCalc' utilities and simplifying maintenance.
Additionally consistency is guaranteed between solver data processing
and post-processing.

The functionObjects have been substantially re-written and generalized
to simplify development and encourage contribution.

Configuration
-------------

An extensive set of simple functionObject configuration files are
provided in

OpenFOAM-dev/etc/caseDicts/postProcessing

and more will be added in the future.  These can either be copied into
'<case>/system' directory and included into the 'controlDict.functions'
sub-dictionary or included directly from 'etc/caseDicts/postProcessing'
using the '#includeEtc' directive or the new and more convenient
'#includeFunc' directive which searches the
'<etc>/caseDicts/postProcessing' directories for the selected
functionObject, e.g.

functions
{
    #includeFunc Q
    #includeFunc Lambda2
}

'#includeFunc' first searches the '<case>/system' directory in case
there is a local configuration.

Description of #includeFunc
---------------------------

    Specify a functionObject dictionary file to include, expects the
    functionObject name to follow (without quotes).

    Search for functionObject dictionary file in
    user/group/shipped directories.
    The search scheme allows for version-specific and
    version-independent files using the following hierarchy:
    - \b user settings:
      - ~/.OpenFOAM/\<VERSION\>/caseDicts/postProcessing
      - ~/.OpenFOAM/caseDicts/postProcessing
    - \b group (site) settings (when $WM_PROJECT_SITE is set):
      - $WM_PROJECT_SITE/\<VERSION\>/caseDicts/postProcessing
      - $WM_PROJECT_SITE/caseDicts/postProcessing
    - \b group (site) settings (when $WM_PROJECT_SITE is not set):
      - $WM_PROJECT_INST_DIR/site/\<VERSION\>/caseDicts/postProcessing
      - $WM_PROJECT_INST_DIR/site/caseDicts/postProcessing
    - \b other (shipped) settings:
      - $WM_PROJECT_DIR/etc/caseDicts/postProcessing

    An example of the \c \#includeFunc directive:
    \verbatim
        #includeFunc <funcName>
    \endverbatim

postProcess
-----------

The 'postProcess' utility and '-postProcess' solver option provide the
same set of controls to execute functionObjects after the run either by
reading a specified set of fields to process in the case of
'postProcess' or by reading all fields and models required to start the
run in the case of '-postProcess' for each selected time:

postProcess -help

Usage: postProcess [OPTIONS]
options:
  -case <dir>       specify alternate case directory, default is the cwd
  -constant         include the 'constant/' dir in the times list
  -dict <file>      read control dictionary from specified location
  -field <name>     specify the name of the field to be processed, e.g. U
  -fields <list>    specify a list of fields to be processed, e.g. '(U T p)' -
                    regular expressions not currently supported
  -func <name>      specify the name of the functionObject to execute, e.g. Q
  -funcs <list>     specify the names of the functionObjects to execute, e.g.
                    '(Q div(U))'
  -latestTime       select the latest time
  -newTimes         select the new times
  -noFunctionObjects
                    do not execute functionObjects
  -noZero           exclude the '0/' dir from the times list, has precedence
                    over the -withZero option
  -parallel         run in parallel
  -region <name>    specify alternative mesh region
  -roots <(dir1 .. dirN)>
                    slave root directories for distributed running
  -time <ranges>    comma-separated time ranges - eg, ':10,20,40:70,1000:'
  -srcDoc           display source code in browser
  -doc              display application documentation in browser
  -help             print the usage

 pimpleFoam -postProcess -help

Usage: pimpleFoam [OPTIONS]
options:
  -case <dir>       specify alternate case directory, default is the cwd
  -constant         include the 'constant/' dir in the times list
  -dict <file>      read control dictionary from specified location
  -field <name>     specify the name of the field to be processed, e.g. U
  -fields <list>    specify a list of fields to be processed, e.g. '(U T p)' -
                    regular expressions not currently supported
  -func <name>      specify the name of the functionObject to execute, e.g. Q
  -funcs <list>     specify the names of the functionObjects to execute, e.g.
                    '(Q div(U))'
  -latestTime       select the latest time
  -newTimes         select the new times
  -noFunctionObjects
                    do not execute functionObjects
  -noZero           exclude the '0/' dir from the times list, has precedence
                    over the -withZero option
  -parallel         run in parallel
  -postProcess      Execute functionObjects only
  -region <name>    specify alternative mesh region
  -roots <(dir1 .. dirN)>
                    slave root directories for distributed running
  -time <ranges>    comma-separated time ranges - eg, ':10,20,40:70,1000:'
  -srcDoc           display source code in browser
  -doc              display application documentation in browser
  -help             print the usage

The functionObjects to execute may be specified on the command-line
using the '-func' option for a single functionObject or '-funcs' for a
list, e.g.

postProcess -func Q
postProcess -funcs '(div(U) div(phi))'

In the case of 'Q' the default field to process is 'U' which is
specified in and read from the configuration file but this may be
overridden thus:

postProcess -func 'Q(Ua)'

as is done in the example above to calculate the two forms of the divergence of
the velocity field.  Additional fields which the functionObjects may depend on
can be specified using the '-field' or '-fields' options.

The 'postProcess' utility can only be used to execute functionObjects which
process fields present in the time directories.  However, functionObjects which
depend on fields obtained from models, e.g. properties derived from turbulence
models can be executed using the '-postProcess' of the appropriate solver, e.g.

pisoFoam -postProcess -func PecletNo

or

sonicFoam -postProcess -func MachNo

In this case all required fields will have already been read so the '-field' or
'-fields' options are not be needed.

Henry G. Weller
CFD Direct Ltd.
2016-05-28 18:58:48 +01:00
Henry Weller
3eec5854be Standardized the selection of required and optional fields in BCs, fvOptions, functionObjects etc.
In most boundary conditions, fvOptions etc. required and optional fields
to be looked-up from the objectRegistry are selected by setting the
keyword corresponding to the standard field name in the BC etc. to the
appropriate name in the objectRegistry.  Usually a default is provided
with sets the field name to the keyword name, e.g. in the
totalPressureFvPatchScalarField the velocity is selected by setting the
keyword 'U' to the appropriate name which defaults to 'U':

        Property     | Description             | Required    | Default value
        U            | velocity field name     | no          | U
        phi          | flux field name         | no          | phi
        .
        .
        .

However, in some BCs and functionObjects and many fvOptions another
convention is used in which the field name keyword is appended by 'Name'
e.g.

        Property     | Description             | Required    | Default value
        pName        | pressure field name     | no          | p
        UName        | velocity field name     | no          | U

This difference in convention is unnecessary and confusing, hinders code
and dictionary reuse and complicates code maintenance.  In this commit
the appended 'Name' is removed from the field selection keywords
standardizing OpenFOAM on the first convention above.
2016-05-21 20:28:20 +01:00
Henry Weller
83bae2efd3 functionObjects: Renamed dictionary entry 'functionObjectLibs' -> 'libs'
This changes simplifies the specification of functionObjects in
controlDict and is consistent with the 'libs' option in controlDict to
load special solver libraries.

Support for the old 'functionObjectLibs' name is supported for backward compatibility.
2016-05-16 22:09:01 +01:00
Henry Weller
274d1df8a4 snappyHexMesh: Automatically remove zero-sized patches
All patches are preserved if the 'keepPatches' option is set true.
Patch contributed by Mattijs Janssens
2016-05-13 17:47:38 +01:00
Henry Weller
6164c2f262 Standardized the naming of functions which control the writing of fields etc.
to have the prefix 'write' rather than 'output'

So outputTime() -> writeTime()

but 'outputTime()' is still supported for backward-compatibility.

Also removed the redundant secondary-writing functionality from Time
which has been superseded by the 'writeRegisteredObject' functionObject.
2016-05-12 17:38:01 +01:00
Henry Weller
c983670c91 functionObjects: Changed options 'outputControl' -> 'writeControl' and 'outputInterval' -> 'writeInterval'
for consistency with the time controls in controlDict and to avoid
unnecessary confusion.  All code and tutorials have been updated.

The old names 'outputControl' and 'outputInterval' are but supported for
backward compatibility but deprecated.
2016-05-12 11:38:11 +01:00
Henry Weller
cf4b35693c tutorials: Remove the unnecessary "\"s on "cp", "rm" and "mv"
Resolves bug-report http://bugs.openfoam.org/view.php?id=2077
2016-05-05 15:17:55 +01:00
Henry Weller
1b34231340 tutorials: Renamed .org -> .orig
See http://www.openfoam.org/mantisbt/view.php?id=2076
  - .org is the file extension for emacs org-mode as well
  - .orig is more to the point (.org isn't always recognized as "original")
  - .original is too long, although more consistent with the convention
    of source code file naming

Update script contributed by Bruno Santos
2016-04-30 21:53:50 +01:00
Henry Weller
e5a029c187 tutorials/multiphase/interDyMFoam/ras/damBreakWithObstacle: Added alphaPhi to correctFluxes
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=2062
2016-04-21 21:19:01 +01:00
Henry Weller
bbc05bdf7e tutorials/multiphase/interDyMFoam/ras/DTCHull: Updated to use the rigidBodyDynamics solver 2016-04-19 10:35:09 +01:00
Henry Weller
d0b5bef948 tutorials/multiphase/interDyMFoam/ras/floatingObject: Updated to use rigidBodyDynamics 2016-04-18 15:41:10 +01:00
Henry Weller
4bc77e6aff Sprucing up the tutorials folder and adding -dict to "collapseEdges"
Patch provided by Bruno Santos
Resolves patch application request http://www.openfoam.org/mantisbt/view.php?id=2015
2016-03-06 19:06:44 +00:00
mattijs
bcb17b23b1 ENH: createPatch: removed createPatch after snappyHexMesh to remove zero-sized patches
This is now handled inside snappyHexMesh with the keepPatches setting.
2016-06-22 11:21:00 +01:00
sergio
6905a80c15 Reordering interDyFoam cases for RAS and laminar 2016-06-14 15:09:59 -07:00
Andrew Heather
16dfd33db8 ENH: Tutorials - updates 2016-04-26 14:32:19 +01:00
Andrew Heather
a7dcf8fc61 ENH: Tutorials - updated use of -log to use -s 2016-04-26 09:31:44 +01:00
Andrew Heather
b9313ef2fe ENH: Consistency updates after Foundation merge and code tidying 2016-04-25 16:46:56 +01:00
andy
fd9d801e2d GIT: Initial commit after latest foundation merge 2016-04-25 11:40:48 +01:00
Henry Weller
350d03246e scripts: Reformat with consistent section separators 2016-02-15 18:30:24 +00:00
Henry Weller
daf44fda3d tutorials and templates: Updated wall BC for velocity to noSlip 2016-02-09 20:08:34 +00:00
Henry Weller
b3d47f0423 bin/tools/RunFunctions: runParallel now obtains the number of processors from numberOfSubdomains
in decomposeParDict.

This default number of processors may be overridden by the new "-np"
option to runParallel which must be specified before the application
name e.g.:

runParallel -np 4 pisoFoam
2016-01-27 14:19:25 +00:00
mattijs
e852970330 ENH: motorBike: tutorial with dynamic refinement across snappyHexMesh mesh 2016-01-21 17:46:40 +00:00
Henry Weller
56fa7c0906 Update code to use the simpler C++11 template syntax removing spaces between closing ">"s 2016-01-10 22:41:16 +00:00
Andrew Heather
f0c3e8d599 STYLE: Updated version to 'plus' 2015-12-22 23:14:17 +00:00
Andrew Heather
04752147c8 GIT: Resolved conflict on merge from upstream 2015-12-22 16:49:44 +00:00
Andrew Heather
0e01c44129 GIT: Resolved conflict 2015-12-09 16:19:28 +00:00
Andrew Heather
5c9dff6146 GIT: Resolved conflict 2015-12-09 16:19:28 +00:00
Andrew Heather
8837a89237 STYLE: Updated links from openfoam.org to openfoam.com 2015-12-09 15:03:05 +00:00
Henry Weller
d98136e122 tutorials: Removed unnecessary "boundary" files 2015-11-13 20:05:37 +00:00
Henry Weller
f4202d9ee6 sixDoFSolver: Run-time selectable solver (integrator) for sixDoFRigidBodyMotion
The built-in explicit symplectic integrator has been replaced by a
general framework supporting run-time selectable integrators.  Currently
the explicit symplectic, implicit Crank-Nicolson and implicit Newmark
methods are provided, all of which are 2nd-order in time:

Symplectic 2nd-order explicit time-integrator for 6DoF solid-body motion:

    Reference:
        Dullweber, A., Leimkuhler, B., & McLachlan, R. (1997).
        Symplectic splitting methods for rigid body molecular dynamics.
        The Journal of chemical physics, 107(15), 5840-5851.

    Can only be used for explicit integration of the motion of the body,
    i.e. may only be called once per time-step, no outer-correctors may be
    applied.  For implicit integration with outer-correctors choose either
    CrankNicolson or Newmark schemes.

    Example specification in dynamicMeshDict:
    solver
    {
        type    symplectic;
    }

Newmark 2nd-order time-integrator for 6DoF solid-body motion:

    Reference:
        Newmark, N. M. (1959).
        A method of computation for structural dynamics.
        Journal of the Engineering Mechanics Division, 85(3), 67-94.

    Example specification in dynamicMeshDict:
    solver
    {
        type    Newmark;
        gamma   0.5;    // Velocity integration coefficient
        beta    0.25;   // Position integration coefficient
    }

Crank-Nicolson 2nd-order time-integrator for 6DoF solid-body motion:

    The off-centering coefficients for acceleration (velocity integration) and
    velocity (position/orientation integration) may be specified but default
    values of 0.5 for each are used if they are not specified.  With the default
    off-centering this scheme is equivalent to the Newmark scheme with default
    coefficients.

    Example specification in dynamicMeshDict:
    solver
    {
        type    CrankNicolson;
        aoc     0.5;    // Acceleration off-centering coefficient
        voc     0.5;    // Velocity off-centering coefficient
    }

Both the Newmark and Crank-Nicolson are proving more robust and reliable
than the symplectic method for solving complex coupled problems and the
tutorial cases have been updated to utilize this.

In this new framework it would be straight forward to add other methods
should the need arise.

Henry G. Weller
CFD Direct
2015-10-19 14:03:46 +01:00
Henry Weller
37cfc3ab46 tutorials: Removed unnecessary spaces between parentheses and values in vectors 2015-07-21 20:55:44 +01:00
Henry Weller
4c21f24a8c Input of dimensionedScalars: update read-construction of dimensionedScalar in applications
so that the specification of the name and dimensions are optional in property dictionaries.

Update tutorials so that the name of the dimensionedScalar property is
no longer duplicated but optional dimensions are still provided and are
checked on read.
2015-07-20 22:52:53 +01:00
Henry Weller
0fb6a01280 fluxRequired: Added setFluxRequired function to fvSchemes class
Added calls to setFluxRequired for p, p_rgh etc. in all solvers which
avoids the need to add fluxRequired entries in fvSchemes dictionaries.
2015-07-15 21:57:16 +01:00
Henry
0a6ca7ae45 includeEtcEntry: New dictionary include directive: #includeEtc "etcFile"
Description
    Specify an etc file to include when reading dictionaries, expects a
    single string to follow.

    Searches for files from user/group/shipped directories.
    The search scheme allows for version-specific and
    version-independent files using the following hierarchy:
    - \b user settings:
      - ~/.OpenFOAM/\<VERSION\>
      - ~/.OpenFOAM/
    - \b group (site) settings (when $WM_PROJECT_SITE is set):
      - $WM_PROJECT_SITE/\<VERSION\>
      - $WM_PROJECT_SITE
    - \b group (site) settings (when $WM_PROJECT_SITE is not set):
      - $WM_PROJECT_INST_DIR/site/\<VERSION\>
      - $WM_PROJECT_INST_DIR/site/
    - \b other (shipped) settings:
      - $WM_PROJECT_DIR/etc/

    An example of the \c \#includeEtc directive:
    \verbatim
        #includeEtc "etcFile"
    \endverbatim

    The usual expansion of environment variables and other constructs is
    retained.
2015-04-26 10:44:11 +01:00
Henry
50ada7c994 blockMesh: Change default location of blockMeshDict from constant/polyMesh to system
For multi-region cases the default location of blockMeshDict is now system/<region name>

If the blockMeshDict is not found in system then the constant directory
is also checked providing backward-compatibility
2015-04-24 22:29:57 +01:00
Henry
e588d61879 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
Henry
5ecfb06398 tutorials: remove unnecessary under-relax fields entry 2015-02-22 16:52:21 +00:00
Henry
74ff779618 tutorials/multiphase/interDyMFoam/ras/floatingObject: Update to demonstrate MULES with Crank-Nicolson 2015-02-22 12:53:34 +00:00
Henry
7be1393fef tutorials: corrected comments in snappyHexMeshDict
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1541
2015-02-17 23:59:59 +00:00
Henry
8628ef2fea Corrected capitalization of Doxygen documentation comments 2015-02-14 13:10:15 +00:00
Henry
1edf292c00 Correct Doxygen multiline comments 2015-02-14 10:59:29 +00:00
Henry
2aec249647 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
Henry
69ff8aa4d2 wallDist: now a MeshObject cached and updated automatically with a run-time selected algorithm
When using models which require the wallDist e.g. kOmegaSST it will
request the method to be used from the wallDist sub-dictionary in
fvSchemes e.g.

wallDist
{
    method meshWave;
}

specifies the mesh-wave method as hard-coded in previous OpenFOAM versions.
2015-01-08 10:40:23 +00:00
Henry
41368addc9 Minor change to comment 2014-12-14 21:50:14 +00:00
OpenFOAM-admin
9fb26d59d3 GIT: Repo update 2014-12-11 08:35:10 +00:00
Henry
0486e20f93 tutorials/multiphase/interDyMFoam/ras/mixerVesselAMI updated 2014-07-24 18:01:08 +01:00
Henry
6a51cc3cbb tutorials: use PIMPLE rather than PISO for rotating mesh problems to ensure updated fluxes are used for momentum transport 2014-07-17 11:34:39 +01:00
mattijs
5fedd93b3d GIT: boundary: remove generated file 2014-07-11 10:53:29 +01:00
Henry
d49889402f sixDoFRigidBodyMotion: Add support to specify the centre for rotation independent of the centre of mass
via the point, line or plane constraints.
2014-05-16 15:35:11 +01:00
Henry
007c694815 DTC tutorial cases: provide reference to original paper
Contains details of case and experimental results
2014-05-09 11:48:37 +01:00
Henry
e6236340b5 Removed alphaOuterCorrectors option because the mass-flux should be updated for all PIMPLE iterations
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1225
2014-03-17 21:31:09 +00:00
Henry
0a7259cc46 Revert pressureInletOutletVelocity BCs
due to convergence problems with the new version for runs at high Courant number
2014-03-12 12:27:19 +00:00
OpenFOAM-admin
fbb3ddf2c4 Updated for release 2.3.0 2014-02-17 10:21:46 +00:00
Henry
a1e778aea3 damBreakWithObstacle: reverted to upwind for U (needs turbulence modelling) and increased Co 2014-02-05 17:18:00 +00:00
Henry
e5e8f49489 damBreakWithObstacle tutorial: changed to linearUpwind 2014-02-05 16:56:45 +00:00
Henry
3e3d30a5a2 twoPhaseEulerFoam tutorials: added minIter to smoothSolver settings 2014-02-05 16:55:34 +00:00
Henry
89f4eca290 interFoam family tutorials: removed redundant and out-of-date alpha entry in fluxRequired 2014-02-05 11:25:05 +00:00
Henry
bd5e4cf172 Default transport solver: change from PBiCG to smoothSolver with symGaussSeidel smoother
Better for most but not all cases.
2014-02-04 16:27:35 +00:00
Henry
54887f6213 Sloshing tutorials: do not update the probe location 2014-02-03 13:05:07 +00:00
Henry
cd764162bf Updated version 2014-02-01 17:18:00 +00:00
Henry
34bc9cadb0 DTCHull: new interDyMFoam tutorial 2014-02-01 17:14:35 +00:00
mattijs
8acfa4692a STYLE: snappyHexMeshDict: removed optional parameter 2014-01-27 12:25:56 +00:00
Henry
a7ad50ce7d VoF tutorials: changed interfaceCompression to linear
This provided greater accuracy and stability while MULES guarantees boundedness
2014-01-23 11:30:45 +00:00
Henry
45b9839203 Updated VoF tutorials 2013-12-21 12:26:32 +00:00
Henry
8af82f02bf sixDoFRigidBodyMotion: remove the constraint and restraint "Coeffs"
sub-dict and put the coefficients in the containing dictionary.
2013-12-15 22:30:52 +00:00
Henry
76ae0daa28 sixDoFRigidBodyMotion/sixDoFRigidBodyMotionSolver: Support restart by caching state in the uniform directory
sixDoFRigidBodyMotionSolver: use point-edge rather than face-cell wave to calculate point distance to surface.
2013-12-10 14:07:27 +00:00
Henry
a09d30dc90 interDyMFoam/ras/floatingObject: apply sixDoFRigidBodyMotion solver
Keep original case as floatingObjectOld
2013-12-08 22:03:56 +00:00
Henry
5ffda9b52b sixDoFRigidBodyMotion: Created separate library
Added sixDoFRigidBodyMotionSolver using septernion interpolation for mesh-morphing
2013-12-08 21:59:40 +00:00
Henry
3f5eda25f0 symmetryPlane: add symmetryPlane as a special type of symmetry condition applied to a single plane
The standard/previous general symmetry type is now named symmetry
    both in class and lookup name for consistency.  The rigorous
    symmetryPlane type is needed for moving-mesh cases in which the
    motion it constrained by one or two planes.
2013-12-06 15:45:11 +00:00
Henry
f8b9abc146 Choose scotch for decomposition 2013-11-10 13:59:54 +00:00
Henry
3e715dfb70 floatingObject
interDyMFoam/ras/floatingObject: Relax the acceleration
2013-11-07 12:23:17 +00:00
Henry
6df8f705ae 6-DoF solid body motion: Support PIMPLE iteration and acceleration relaxation 2013-10-31 10:22:26 +00:00
andy
67a49d125d ENH: Tutorial Allclean script updates 2013-10-11 12:41:11 +01:00
Henry
ff3a4ee345 Improved schemes 2013-09-17 15:56:57 +01:00
mattijs
e9bfae1ac8 BUG: Allrun: incorrect naming 2013-09-13 10:01:00 +01:00
mattijs
121e4346a4 ENH: mixerVesselAMI: split into Allrun and Allrun.pre 2013-09-13 09:51:22 +01:00
mattijs
70624fb740 BUG: U: use uniformFixedValue instead of fixedValue 2013-09-11 12:56:05 +01:00
mattijs
2f8cdf714c BUG: damBreakWithObstacle: unused files 2013-09-11 12:53:34 +01:00
Henry
e2a043d010 Tutorials: removed unnecessary entries from fixedFluxPressure BC specs 2013-09-11 09:49:46 +01:00
Henry
08baa6eda6 fixedFluxPressure BC: the snGrad is now pushed into the BC from pEqn.H rather than being evaluated in the BC 2013-09-11 00:10:00 +01:00
Henry
51f085faa5 Rewrite of ddtPhiCorr - ddtCorr and density-weight HbyA on compressible solvers.
For DyM solvers phiAbs is replaced by Uf but this conversion is currently not complete
2013-09-09 12:41:20 +01:00
Henry
005bfcd851 multiphase: completed renaming of phase fields to use the new groupName convention and interface 2013-08-22 16:51:16 +01:00
Henry
2780df8365 multiphase: Update phase-naming to use the new convention e.g. alpha.water 2013-08-13 23:21:46 +01:00
mattijs
f196efa6d7 GIT: boundary: generated file 2013-08-07 12:27:48 +01:00
Henry
f75138d1f6 solidBodyMotionFunctions: Changed CofG to origin where appropriate and support run-time selectable omega specification in rotatingMotion 2013-07-30 09:41:27 +01:00
Henry
03b60c81d0 Remove unnecessary files 2013-07-15 14:46:58 +01:00
Henry
1522a5e178 Update version 2013-07-15 14:46:06 +01:00
Henry
109ecd88b5 tutorials/multiphase/interDyMFoam/ras/mixerVesselAMI: mixer vessel AMI VoF tutorial 2013-07-15 14:43:32 +01:00
Henry
052d81785a multiphase: move alpha solution controls into the appropriate sub-dictionary of fvSolution:solvers 2013-06-20 16:32:39 +01:00
Henry
a114345eab Thermodynamics and sub-models: Removed "Sp" boundedness corrections on transport, replaced with "bounded Gauss" scheme 2012-09-21 14:34:42 +01:00
mattijs
74e0e13104 BUG: controlDict: writeInterval syntax 2012-09-20 14:47:33 +01:00
mattijs
93ee8749e9 BUG: controlDict: writeInterval syntax 2012-09-20 14:47:02 +01:00
mattijs
bfbfa8f4a5 ENH: motionSolvers: dynamicMeshDict new syntax 2012-08-31 16:51:26 +01:00
Henry
c1d61707b6 interDyMFoam tutorials: use phiAbs for P BCs 2012-08-02 16:33:32 +01:00
Henry
1464c4ff5c multiphase (VoF): Added support for general turbulence models
Required the addition of the divDevRhoR function to all incompressible turbulence models
2012-07-27 14:56:01 +01:00
Henry
ef8efc27ba Solvers and tutorials: changed use of buoyantPressure BC to fixedFluxPressure 2012-04-20 09:49:58 +01:00
Henry
2491f257b1 Corrected line lengths 2012-02-29 16:39:53 +00:00
Henry
52d5229be4 interDyMFoam floatingObject tutorial: update relaxation factors 2012-01-31 11:19:36 +00:00