Moved part common to all derived classes (e.g. update) to the base
class to avoid code duplication. Practically, only the protected
updateDesignVariables has to be overwritten in each derived class now.
steadyOptimisation was also affected in a minor way.
- Added function returning the underlaying surface sensitivities
- Added boolean to control whether to write the underlaying sensitivity
map (defaults to false)
Encapsulates all terms that are common in both E(SI) and FI
formulations, like direct sensitivities and sensitivities due to
primal boundary conditions. Added the latter to all derived sensitivity
types, except for sensitivity maps.
Same as adjointWallVelocity but also returns the contribution
of the differentiation of the rotatingWallVelocity BC wrt the
face centres, to be added to the sensitivity derivatives.
Main reason was the insertion of a templated virtual function
returning the contribution of the differentiation of the primal
boundary condition, in the case the latter directly depends on a
a geometric quantity (e.g. rotatingWallVelocity).
Example usage:
removeParcels1
{
type removeParcels;
log yes;
resetOnWrite no;
resetOnStart no;
faceZones (cycLeft cycRight);
}
Number and mass of particles removed are written to file
to geometricVoF
sampledInterface was linked to interfaceProperties thorugh geometricVoF,
and interfaceProperties created a conflict on surfaceTension table
when linked in the reactingEuler solvers by the sampling lib
Example usage:
cloudFunctions
{
WeberNumber1
{
type WeberNumber;
}
}
This will calculate and write the Weber number field as a 'standard'
cloud field, available for post-processing alongside other lagrangian
fields in the lagrangian/<cloudName> directory.
ENH: add log FO
ENH: improve log with scale, and offset entries
BUG: ensure extrueMesh does not fail in parallel with wedge extrusion
BUG: add missing clone and mapping funcs to copiedFixedValue, fixedMultiPhaseHeatFlux
ENH: meshToMesh0::cellAddressing slight speed up for some geometries
BUG:0003495: Divide-by-zero in SHF particle break-up model
BUG:0003492: The formula in the OF is inconsistent with the Rosin-Rammler distribution theory formula
- replace ':' scoping with IOobject::scopedName(), which automatically
uses '_' for Windows compilations where the ':' is a meta-character
(drive separator)
- apply similar local change for the momentum function object.
*** This topic will be revisited in the future ***
Please refer to the header file documentation for complete set of details.
ENH: add new fvOptions for ABL modelling
- atmAmbientTurbSource
- atmBuoyancyTurbSource
- atmCoriolisUSource
- atmLengthScaleTurbSource
- atmPlantCanopyTurbSource
- atmPlantCanopyUSource
- atmPlantCanopyTSource
- atmNutSource
ENH: add new boundary conditions for ABL modelling
with PatchFunction1 and TimeFunction1 support
- atmAlphatkWallFunction
- atmEpsilonWallFunction
- atmNutkWallFunction
- atmNutUWallFunction
- atmNutWallFunction
- atmOmegaWallFunction
- atmTurbulentHeatFluxTemperature
STYLE: change names of nutkAtmRoughWallFunction -> atmNutkWallFunction by
ensuring the bitwise backward compatibility
ENH: add new variable-scaling force computation method to actuationDiskSource
ENH: review actuationDiskSource and radialActuationDiskSource
ENH: add new function object, ObukhovLength
ENH: add new ABL tutorials/verifications
- verificationAndValidation/atmosphericModels/atmFlatTerrain
- verification with the Leipzig field experiment
- illustration of precursor/successor field mapping
- verificationAndValidation/atmosphericModels/atmForestStability
- verification with the Sweden field experiment
- update incompressible/simpleFoam/turbineSiting
1) Implementation of the compressibleIsoInterFOam solver
2) Implementation of a new PLIC interpolation scheme.
3) New tutorials associated with the solvers
This implementation was carried out by Henning Scheufler (DLR) and Johan
Roenby (DHI), following :
\verbatim
Henning Scheufler, Johan Roenby,
Accurate and efficient surface reconstruction from volume fraction data
on general meshes, Journal of Computational Physics, 2019, doi
10.1016/j.jcp.2019.01.009
\endverbatim
The integration of the code was carried out by Andy Heather and Sergio
Ferraris from OpenCFD Ltd.
ENH: update libs of etc/caseDicts/postProcess items
ENH: ensure destructor=default
ENH: ensure constness
ENH: ensure no 'copy construct' and 'no copy assignment' exist
TUT: add examples of function objects with full set
of settings into a TUT if unavailable
TUT: update pisoFoam/RAS/cavity tutorial in terms of usage
The PIMPLE option finalOnLastPimpleIterOnly allows the call the Final
solver only in the last PIMPLE loop. The default is false which is
the present behavior.
- When compiling additional modules or user code, we need more control
for the installation locations beyond the usual FOAM_USER_LIBBIN,
FOAM_SITE_LIBBIN, FOAM_LIBBIN, and wish to have these values be
modifiable without editing files.
- provide wmake rules for handling standard defaults:
* GENERAL_RULES/module-path-user
* GENERAL_RULES/module-path-group
* GENERAL_RULES/module-path-project
which are incorporated as follows:
Make/options:
include $(GENERAL_RULES)/module-path-user
Make/files:
LIB = $(FOAM_MODULE_LIBBIN)/libMyLibrary
By default these would compile into FOAM_USER_{APPBIN,LIBBIN} but
could be adjusted at compilation time. For example,
```
wmake -module-prefix=/path/my-install-location
```
Or
```
./Allwmake -module-prefix=/path/my-install-location
./Allwmake -prefix=/path/my-install-location
```
Or
```
FOAM_MODULE_PREFIX=/path/my-install-location ./Allwmake
```
ENH: add -no-recursion option for AllwmakeParseArguments
- more descriptive naming than the -fromWmake option (still supported)
- remove wmake/scripts/wmake.{cmake,wmake}-args since the -prefix
handling and -no-recursion is now directly handled by AllwmakeParseArguments
ENH: add generalised log-law type ground-normal inflow boundary conditions for
wind velocity and turbulence quantities for homogeneous, two-dimensional,
dry-air, equilibrium and neutral atmospheric boundary layer (ABL) modelling
ENH: remove `zGround` entry, which is now automatically computed
ENH: add `displacement height` entry, `d`
ENH: add generalised atmBoundaryLayerInletOmega boundary condition
ENH: add a verification case for atmBoundaryLayerInlet BCs
DOC: improve atmBoundaryLayerInlet header documentation
BUG: fix value-entry behaviour in atmBoundaryLayerInlet (fixes#1578)
Without this change:
- for serial-parallel computations, if `value` entry is available in
an `atmBoundaryLayerInlet` BC, the theoretical ABL profile expressions
are not computed, and the `value` entry content is used as a profile data
- for parallel computations, if `value` entry is not available, `decomposePar`
could not be executed.
With this change:
- assuming `value` entry is always be present, the use of `value` entry for
the ABL profile specification is determined by a flag `initABL`
- the default value of the optional flag `initABL` is `true`, but whenever
`initABL=true` is executed, `initABL` is overwritten as `false` for the
subsequent runs, so that `value` entry can be safely used.
Thanks Per Jørgensen for the bug report.
BUG: ensure atmBoundaryInlet conditions are Galilean-invariant (fixes#1692)
Related references:
The ground-normal profile expressions (tag:RH):
Richards, P. J., & Hoxey, R. P. (1993).
Appropriate boundary conditions for computational wind
engineering models using the k-ε turbulence model.
In Computational Wind Engineering 1 (pp. 145-153).
DOI:10.1016/B978-0-444-81688-7.50018-8
Modifications to preserve the profiles downstream (tag:HW):
Hargreaves, D. M., & Wright, N. G. (2007).
On the use of the k–ε model in commercial CFD software
to model the neutral atmospheric boundary layer.
Journal of wind engineering and
industrial aerodynamics, 95(5), 355-369.
DOI:10.1016/j.jweia.2006.08.002
Expression generalisations to allow height
variation for turbulence quantities (tag:YGCJ):
Yang, Y., Gu, M., Chen, S., & Jin, X. (2009).
New inflow boundary conditions for modelling the neutral equilibrium
atmospheric boundary layer in computational wind engineering.
J. of Wind Engineering and Industrial Aerodynamics, 97(2), 88-95.
DOI:10.1016/j.jweia.2008.12.001
The generalised ground-normal profile expression for omega (tag:YGJ):
Yang, Y., Gu, M., & Jin, X., (2009).
New inflow boundary conditions for modelling the
neutral equilibrium atmospheric boundary layer in SST k-ω model.
In: The Seventh Asia-Pacific Conference on Wind Engineering,
November 8-12, Taipei, Taiwan.
Reproduced benchmark:
Rectangular prism shown in FIG 1 of
Hargreaves, D. M., & Wright, N. G. (2007).
On the use of the k–ε model in commercial CFD software
to model the neutral atmospheric boundary layer.
Journal of wind engineering and
industrial aerodynamics, 95(5), 355-369.
DOI:10.1016/j.jweia.2006.08.002
Benchmark data:
HW, 2007 FIG 6
TUT: update simpleFoam/turbineSiting tutorial accordingly
STDMD (i.e. Streaming Total Dynamic Mode Decomposition) is a variant of
a data-driven dimensionality reduction method.
STDMD is being used as a mathematical post-processing tool to compute
a set of dominant modes out of a given flow (or dataset) each of which is
associated with a constant frequency and decay rate, so that dynamic
features of a given flow may become interpretable, and tractable.
Among other Dynamic Mode Decomposition (DMD) variants, STDMD is presumed
to provide the general DMD method capabilities alongside economised and
feasible memory and CPU usage.
Please refer to the header file documentation for further details.
ENH: add new STDMD tutorial, pimpleFoam/laminar/cylinder2D
ENH: add Test-EigenMatrix application
The new iterative eigen decomposition functionality is
derived from:
Passalacqua et al.'s OpenQBMM (openqbmm.org/),
which is mostly derived from JAMA (math.nist.gov/javanumerics/jama/).
