- now mark methods with strict deprecation, to make it easier to find
their use but without adding extra compilation noise for others
ENH: minor update for Enum methods and iterator
- add warnOnly (failsafe) option for readEntry and getOrDefault
- add good() method to Enum iterator (simliar to HashTable)
- replace unused/fragile Enum find() methods with iterator return
that can be used more generally
- update TimeState access methods
- use writeTime() instead of old method name outputTime()
- use deltaTValue() instead of deltaT().value()
to avoids pointless construct of intermediate
- initialise with Switch::INVALID and then test if good() to
trigger the initial update.
This avoids some overhead, but primarily avoids ambiguity with
implicit casting to a 'bool' that autoPtr<bool> has.
In the 'standard' and 'UaGradU' options for the ATC term of the adjoint
equations, there is an option to add 'aritificial dissipation', by
adding and subtracting a multiple of the adjoint convection term with
different discretizations. The implicit part was not multiplied with the
ATClimiter whereas the explicit one was, leading to mismatched
contributions in the areas affected by the ATClimiter, which could
affect the sensitivity derivatives.
- reduces clutter. In some cases the Fwd typedefs were also incorrect
STYLE: combine Scalar specialisations into corresponding PatchFields.C
- reduces clutter, simplifies future adjustments
- flowRate: volume flow-rate through given patches
- flowRatePartition: distribution of the inlet flow-rate to certain
outlet patches, with given percentages
- uniformityPatch: uniformity of the velocity field at given (outlet) patches,
expressed as (half) the variance of the velocity field
- uniformityCellZone: same as uniformityPatch, but defined over
cellZones
- powerDissipation: the fluid power dissipation taking place within
given cellZones. In the absence of viscous stress at the "inlets" and
"outlets" of the cellZones, this corresponds to the volume flow-rate
weighted total pressure losses through the cellZones
ENH: updated nutSqr so it can be used with adjointkOmegaSST too
to help allocate pointers related to contributions to the adjoint
turbulence model PDEs, populate them and check the validity of the
cellZones provided for cellZone-based objectives
- avoids redundant dictionary searching
STYLE: remove dictionary lookupOrDefaultCompat wrapper
- deprecated and replaced by getOrDefaultCompat (2019-05).
The function is usually specific to internal keyword upgrading
(version compatibility) and unlikely to exist in any user code.
STYLE: qualify format/version/compression with IOstreamOption not IOstream
STYLE: reduce number of lookups when scanning {fa,fv}Solution
STYLE: call IOobject::writeEndDivider as static
in RASModelVariables were doing this by checking whether the
corresponding pointer was allocated. In some cases, however, even if the
field does not exist, the pointer is not null, leading to the wrong
output. Made the correspding functions virtual and overwritten their
return values in the derived classes. Kept the initial implementation in
base to facilitate the clone function.
in cases with more than one primal or adjoint solvers
TUT: removed all occurances of useSolverNameForFields
from the optimisation tutorials since it is now set
automatically.
in the sensitivity patches, symmetry::evaluate() needs access to the
internalField which does exist, leading to wrong memory access.
Fixed by specifying a calculated type fvPatchField for all patches when
creating a boundaryField<Type>
Using a symmetry(Plane) as a sensitivity patch is quite rare and
borderline wrong, but this provides a fix nonetheless.
The multiplier of grad(dxdb) is a volTensorField which, by itself, is
memory consuming. The function computing it though was sloppy in terms
of memory management, constituting the peak memory consumption during an
adjoint optimisation. Initial changes to remedy the problem include the
deallocation of some of the volTensorFields included in the computation
of grad(dxdb) once unneeded, the utilisation of volSymmTensorFields
instead of volTensorFields where possible and avoiding allocating some
unnecessary intermediate fields.
Actions to further reduce memory consumption:
- For historical reasons, the code computes/stores the transpose of
grad(dxdb), which is then transposed when used in the computation of
the FI or the ESI sensitivity derivatives. This redundant
transposition can be avoid, saving the allocation of an additional
volTensorField, but the changes need to permeate a number of places in
the code that contribute to grad(dxdb) (e.g. ATC, adjoint turbulence
models, adjoint MRF, etc).
- Allocation of unnecessary pointers in the objective class should be
avoided.
- ATCstandard, ATCUaGradU:
the ATC is now added as a dimensioned field and not as an fvMatrix
to UaEqn. This get rid of many unnecessary allocations.
- ATCstandard:
gradU is cached within the class to avoid its re-computation in
every adjoint iteration of the steady state solver.
- Inlined a number of functions within the primal and adjoint solvers.
This probably has a negligible effect since they likely were inlined
by the compiler either way.
- The momentum diffusivity at the boundary, used by the adjoint boundary
conditions, was computed for the entire field and, then, only the
boundary field of each adjoint boundary condition was used. If many
outlet boundaries exist, the entire nuEff field would be computed as
many times as the number of boundaries, leading to an unnecessary
computational overhead.
- Outlet boundary conditions (both pressure and velocity) use the local
patch gradient to compute their fluxes. This patch gradient requires
the computation of the adjacent cell gradient, which is done on the
fly, on a per patch basis. To compute this patch adjacent gradient
however, the field under the grad sign is interpolated on the entire
mesh. If many outlets exist, this leads to a huge computational
overhead. Solved by caching the interpolated field to the database and
re-using it, in a way similar to the caching of gradient fields (see
fvc::grad).
WIP: functions returning references to primal and adjoint boundary
fields within boundaryAdjointContributions seem to have a non-negligible
overhead for cases with many patches. No easy work-around here since
these are virtual and cannot be inlined.
WIP: introduced the code structure for caching the contributions to
the adjoint boundary conditions that depend only on the primal fields
and reusing. The process needs to be completed and evaluated, to make
sure that the extra code complexity is justified by gains in
performance.
is now appended by the name of the adjoint solver, if more than one
exist. This was necessary for an accurate continuation since, before
these changes, only the ma field of the last solver was written. As a
result, when restarting the first adjoint solver was reading the ma
field of the last one. No changes are needed in fvSolution and fvSchemes
w.r.t. the previous code version.
as a step towards machine-accuracy continuation of the optimisation
loop.
Additionally, control points are now written under the time/uniform
folder, to be in-line with rest of the code structure for continuation.
As a side-effect, the controlPointsDefinition in
constant/dynamicMeshDict does not need to be changed to 'fromFile'
anymore in order to perform the continuation. The 'fromFile' option is
still valid if the user wants to supply the control points manually but,
as with all other controlPointsDefinitions, it will be disregarded if the
proper file exists under the time/uniform/volumetricBSplines folder.
Before the commit, the sensitivity classes were receiving references of
the (incompressible) primal and adjoint variables. However, if
additional physics was added (energy equation, multiphase, etc), the
infrastructure wasn't convenient for accommodating (new terms in the FI
and E-SI formulations, new terms in the sensitivity map, etc).
Now, the sensitivity classes receive a reference to an
incompressibleAdjointSolver and receive the terms for the FI and
sensitivity maps through there. The latter is still WIP.
Modified adjointSimple to incorporate these changes as well.
Each solver now writes its sensitivity derivatives to its dictionary,
enabling also a binary format. If present, the sensitivities are then
re-read from the dictionary, avoiding thus possible loss of information
due to re-computation.
As a side-effect, sensitivities are computed after the completion of
each adjoint solver, instead of being computed after all adjoint solvers
have been completed.
for incompressible flows. The typical convention of appending the primal
field name with 'a' to form the adjoint field is followed for the
adjoint turbulent kinetic energy (i.e. 'ka') but since this would produce
an ugly variable name for the adjoint to omega (i.e. omegaa), the latter
is abbreviated to 'wa'.
The work is based on
\verbatim
Kavvadias, I., Papoutsis-Kiachagias, E.,
Dimitrakopoulos, G., & Giannakoglou, K. (2014).
The continuous adjoint approach to the k–$omega$ SST turbulence model with
applications in shape optimization
Engineering Optimization, 47(11), 1523-1542.
https://doi.org/10.1080/0305215X.2014.979816
\endverbatim
with changes in the discretisation of
a number of differential operators and the formulation of the adjoint to
the wall functions employed by the primal model.
Regarding the latter, the code assumes (and differentiates) the default
behaviour of nutkWallFunction (i.e. nutWallFunction::blendingType::STEPWISE)
and omegaWallFunction (i.e. omegaWallFunction::blendingType::BINOMIAL2).
Due to the availability of a number of terms required for the
formulation of the wall function for ka, the latter is implemented
within adjointkOmegaSST itself, with contributions from objective functions
implemented within kaqRWallFunction. Wall functions for wa are
implemented within waWallFunction.
The initial implementation of the above-mentioned reference was
performed by Dr. Ioannis Kavvadias
the Jacobian of an objective function, defined at the boundary, wrt nut
and gradU. Also modified the current objectives that include such
contributions
