Commit Graph

19 Commits

Author SHA1 Message Date
b55bc28698 sampledSurface::writers: Added writeFormat option to select ascii or binary
e.g. in tutorials/incompressible/pisoFoam/LES/motorBike/motorBike/system/cuttingPlane

    surfaceFormat   vtk;
    writeFormat     binary;
    fields          (p U);

selects writing the VTK surface files in binary format which significantly
speeds-up reading of the files in paraview.

Currently binary writing is supported in VTK and EnSight formats.
2020-01-29 14:59:31 +00:00
5f22607df3 tutorials/*/DTCHull, propeller: Clone meshes, if available
These cases now check for a mesh in geometrically identical cases and
copy rather than re-generate if possible. This reduces the run-time of
the test loop by about 20 minutes.
2019-11-04 11:40:40 +00:00
627f1810f4 tutorials::DTCHull: No need to renumber fields before setFields 2019-08-22 21:35:00 +01:00
5acfe8b20a reactingMixture: Rationalised the reading of the species thermo and reactions
which are now read directly from the thermophysicalProperties dictionary for
consistency with non-reacting mixture thermodynamics.  The species thermo and
reactions lists can still be in separate files if convenient and included into
the thermophysicalProperties file using the standard dictionary #include.
2019-08-02 22:47:45 +01:00
784244790f DTCHull tutorials: rename fields to .orig
to avoid them being overwritten during renumbering
2019-04-29 19:26:50 +01:00
1909f9cf85 DTCHull tutorials: renumberMesh after meshing, before decomposition
Avoids the need to renumber the decompositon/reconstruction maps
2019-04-05 17:01:13 +01:00
19c3584d4b functionObject::timeControl: Rationalised naming timeStart -> startTime, timeEnd -> endTime
Support for timeStart and timeEnd is maintained for backward-compatibility but
these names are deprecated.
2019-01-18 13:41:08 +00:00
5bba828399 tutorials/wave: Removed obsolete arguments from setWaves 2018-12-18 12:10:57 +00:00
5925868fb7 waves: Moved mean velocity specification back into the wave models
With the inclusion of boundary layer modelling in the gas, the
separation of wave perturbation from and mean flow became less useful,
and potentially prevents further extension to support similar boundary
layer modelling in the liquid.

The mean velocity entry, UMean, is now needed in the
constant/waveProperties file rather than in the waveVelocity boundary
condition.
2018-12-18 10:34:40 +00:00
967edc9425 waves: Split mean flow from wave perturbation modelling
In order to increase the flexibility of the wave library, the mean flow
handling has been removed from the waveSuperposition class. This makes
waveSuperposition work purely in terms of perturbations to a mean
background flow.

The input has also been split, with waves now defined as region-wide
settings in constant/waveProperties. The mean flow parameters are sill
defined by the boundary conditions.

The new format of the velocity boundary is much simpler. Only a mean
flow velocity is required.

    In 0/U:

        boundaryField
        {
            inlet
            {
                type            waveVelocity;
                UMean           (2 0 0);
            }
            // etc ...
        }

Other wave boundary conditions have not changed.

The constant/waveProperties file contains the wave model selections and
the settings to define the associated coordinate system and scaling
functions:

    In constant/waveProperties:

        origin          (0 0 0);
        direction       (1 0 0);
        waves
        (
            Airy
            {
                length      300;
                amplitude   2.5;
                phase       0;
                angle       0;
            }
        );
        scale           table ((1200 1) (1800 0));
        crossScale      constant 1;

setWaves has been changed to use a system/setWavesDict file rather than
relying on command-line arguments. It also now requires a mean velocity
to be specified in order to prevent ambiguities associated with multiple
inlet patches. An example is shown below:

    In system/setWavesDict:

        alpha   alpha.water;
        U       U;
        liquid  true;
        UMean   (1 0 0);
2018-12-10 13:39:06 +00:00
2e1e8837c0 outletPhaseMeanVelocity: Renamed Umean to UnMean
This is to make it clear that the value supplied is the scalar mean
velocity normal to the patch, and to distinguish it from other instances
of the keyword "UMean" which take a vector quantity.
2018-12-10 09:05:30 +00:00
c3fbcd7398 tutorials/multiphase/interFoam/RAS/DTCHull.*: Simplified U specification using the new #neg function 2018-08-01 09:44:16 +01:00
fdbf3c134f Rationalized dictionary and configuration file headers 2018-07-09 15:40:05 +01:00
bf54ab67e1 Updated OpenFOAM Foundation web-link in headers 2018-07-06 21:42:54 +01:00
019ae8bab3 tutorials: Changed compressed ascii output to binary to improve IO performance
also rationalized the writeCompression specification
2018-06-27 15:25:52 +01:00
0335250577 tutorials: Removed temporary cellMap files 2018-05-31 16:49:29 +01:00
aea8dc0516 tutorials: Updated to use surfaceFeatures rather than the deprecated surfaceFeatureExtract 2018-05-29 19:18:53 +01:00
9221dd0d0f tutorials: Removed 0.orig directories in favor of <field>.orig
The new automated <field>.orig reading has made 0.orig directories and
associated scripting redundant.
2018-02-15 20:14:27 +00:00
46704f121b interFoam: Merged dynamic mesh functionality of interDyMFoam into interFoam
and replaced interDyMFoam with a script which reports this change.

The interDyMFoam tutorials have been moved into the interFoam directory.

This change is one of a set of developments to merge dynamic mesh functionality
into the standard solvers to improve consistency, usability, flexibility and
maintainability of these solvers.

Henry G. Weller
CFD Direct Ltd.
2017-11-30 23:56:42 +00:00