this is only relevant people who are masochistic enough to go beyond
`-Wall`. (note that at this warning level, there is plenty of noise from
Dune and other upstream dependencies.)
further, this cleans up the code of the parameter system and the
startup routines a bit and finally, it adds positional parameters
support to ebos as well as brief descriptions to ebos and the lens
problem.
Dune::set_singularity_limit() was removed and the ILU preconditioners
seem to have been refactored. The ILU refactoring included making the
order of the preconditioner a template parameter of the preconditioner
class, i.e., it can no longer be specified at runtime.
Note that the AMG code in the dune master currently produces quite a
few warnings because of the latter point, but as far as I can see,
there is nothing which can be done about this from outside of
dune-istl.
IMO the term "vanguard" expresses better what these classes are
supposed to do: level the ground for the cavalry. Normally this simply
means to create and distribute a grid object, but it can become quite
a bit more complicated, as exemplified by the vanguard classes of
ebos..
instead of passing a "minimal" fluid state that defines the
thermodynamic conditions on the domain boundary and the models
calculating everything they need based on this, it is now assumed that
all quantities needed by the code that computes the boundary fluxes
are defined. This simplifies the boundary flux computation code, it
allows to get rid of the `paramCache` argument for these methods and
to potentially speed things up because quantities do not get
re-calculated unconditionally.
on the flipside, this requires slightly more effort to define the
conditions at the boundary on the problem level and it makes it less
obvious which quantities are actually used. That said, one now has the
freedom to shoot oneself into the foot more easily when specifying
boundary conditions and also tools like valgrind or ASAN will normally
complain about undefined quantities if this happens.
according to wikipedia the term "heat" is the energy transferred due
to a temperature gradient, i.e., it only makes sense if such a
gradient is present and this is not necessary for the storage term.
this means that technically the term "heat conductivity" is
meaningful, but "thermal conductivity" is IMO more consistent.
this has partially already been done in opm-material and eWoms it was
pretty inconsistent, so it also requires a patch in opm-material.
it broke because of the recent refactoring of the energy material laws
in opm-material. The reason why nobody noticed is that this test
requires dune-alugrid to be compiled.
there seems to be only a *very* limited amount of interest, the code
of the model is quite complex and there are currently no suitable
discretizations for free-flow equations in eWoms (i.e., the model
tends to be very unstable and oscillates a lot). Combined, all of this
makes maintaining this model a pain in the back, so let's remove it
some interest in these kinds of problems surfaces and until
appropriate discretizations -- like staggered grid methods -- are
available.
This works by having a "focus degree of freedom" during
linearization. When evaluating the local residual, all derivatives of
the residual/fluxes are with regard to the primary variables of that
DOF.
The two main offenders were the Forchheimer velocity model and the
model for the Stokes equations. To ensure that they continue to work,
the "powerinjection" and the "stokestest2c" problems are now both
compiled and tested with both, automatic differentiation and finite
differences, and the results of these tests is compared against the
same reference solution.
The majority of the time required to develop this patch was actually
required for testing: All tests compile and pass with debugging and
aggressive optimization flags with at least GCC 5, GCC 7 and clang
3.8, as well as Dune 2.3 and 2.4. Also, the results of flow_ebos stay
identical for Norne whilst the performance difference is below the
measurement noise on my machine. (the version with this patch applied
was actually about 1% faster.)
the groundwater problem should be symmetric because it uses an
incompressible fluid, is a single phase problem and uses the
immiscible model. (i.e., there should never be a difference between
the upstream and the downstream cells.)
the main purpose of this commit is to have a test that uses a linear
solver wrapper which was generated by the internal
EWOMS_WRAP_ISTL_SOLVER macro.
... and use the restarted GMRES solver in conjunction with a ILU-2
preconditioner for the water-air unit test.
I do not really recommend using these solvers because BiCGSTAB tends
to be 20% to 30% slower than our home-brewn implementation (this is
because the dune-istl solvers cannot use custom convergence criteria),
but dune-istl offers more choices than just BiCGStab and this
functionallity could be helpful when debugging issues related to
solving the linear systems of equations.
Note that regardless of how pedantic the interpretation of DUNE's
license is, there are no licensing issues with this code because we do
not distribute any files derived from DUNE anymore.
i.e., the solvers.hh file is removed. The main reason for this is that
it avoids having to distribute a file with a potentially incompatible
license (i.e., GPLv2 + template exception vs GPLv2+), but the
home-brewn bicgstab solver also seems to perform a tiny bit better.
i.e., using clang 3.8 to compile the test suite with the following
flags:
```
-Weverything
-Wno-documentation
-Wno-documentation-unknown-command
-Wno-c++98-compat
-Wno-c++98-compat-pedantic
-Wno-undef
-Wno-padded
-Wno-global-constructors
-Wno-exit-time-destructors
-Wno-weak-vtables
-Wno-float-equal
```
should not produce any warnings anymore. In my opinion the only flag
which would produce beneficial warnings is -Wdocumentation. This has
not been fixed in this patch because writing documentation is left for
another day (or, more likely, year).
note that this patch consists of a heavy dose of the OPM_UNUSED macro
and plenty of static_casts (to fix signedness issues). Fixing the
singedness issues were quite a nightmare and the fact that the Dune
API is quite inconsistent in that regard was not exactly helpful. :/
Finally this patch includes quite a few formatting changes (e.g., all
occurences of 'T &t' should be changed to `T& t`) and some fixes for
minor issues which I've found during the excercise.
I've made sure that all unit tests the test suite still pass
successfully and I've made sure that flow_ebos still works for Norne
and that it did not regress w.r.t. performance.
(Note that this patch does not fix compiler warnings triggered `ebos`
and `flow_ebos` but only those caused by the basic infrastructure or
the unit tests.)
v2: fix the warnings that occur if the dune-localfunctions module is
not available. thanks to [at]atgeirr for testing.
v3: fix dune 2.3 build issue
10^-4 lead to sporadic results if the final tolerance of the solution
really was 10^-4. (it currently is usually better because each time
step experiences an additional update after the Newton method deems it
to be converged.)
this problem did not work properly anyway: it oscillated like hell
(very likely to the spatial discretization used being inappropriate)
and it did not even converge if more than a single iteration was
required.
these are:
- remove the unused methods "baseEpsilon()" and "numericEpsilon()"
from FvBaseAdLocalLinearizer. (they are only meaningful in the
context of finite differences.)
- correct/update some comments
- replace most occurences of Toolbox::createConstant() with
assignments to floating point values to unclutter the code a bit.
this broke with 94006531. I actually fixed the reservoir problem
yesterday before pushing 94006531 but forgot to include the fix in my
local branch before pushing. Stupid me!
now, the dune-alugrid module is required if these tests are to be
run. (note that due to the fact that the OPM build system has not been
detecting the legacy alugrid library for a while, the practical
implications of this patch should be small to non-existant.)
this is necessary to allow non-trivial ParameterCache objects with
Local-AD evaluations. So far, the only fluid system in opm-material
which needs this is the Spe5 fluid system (which is unused by eWoms),
but sooner or later this change would have been required anyway.
Note that it is possible that this patch is errornous if Evaluation !=
Scalar for a fluid system that uses a non-trivial ParameterCache
object, but the errors should be relatively easy to fix...
the in-file lists of authors has been removed in favor of a global
list of authors in the LICENSE file. this is done because (a)
maintaining a list of authors at the beginning of a file is a major
pain in the a**, (b) the list of authors was not accurate in about 85%
of all cases where more than one person was involved and (c) this list
is not legally binding in any way (the copyright is at the person who
authored a given change, if these lists had any legal relevance, one
could "aquire" the copyright of the module by forking it and removing
the lists...)
the only exception of this is the eWoms fork of dune-istl's solvers.hh
file. This is beneficial because the authors of that file do not
appear in the global list. Further, carrying the fork of that file is
required because we would like to use a reasonable convergence
criterion for the linear solver. (the solvers from dune-istl do
neither support user-defined convergence criteria not do the
developers want support for it. (my patch was rejected a few years
ago.))
the changes enable the storage cache and the intensive quantity cache
for all simulators of the lens problem and automatic differentiation
for the one which uses the ECFV discretization.
while the performance improvements are not worthwhile for the problem
in its default incarnation (using automatic diffentiation even
slightly degrades performance), it speeds up linearization by about
30% if the grid exhibits 16 times as many elements (e.g. by passing
the --grid-global-refinements=2) parameter.
at least, they compile as far as eWoms is concerned. Some external
libraries (in particular everything which uses SuperLU) still have
issues.
Also, there seem to be issues with the precision that is achievable
by the Newton method when using float.
this is because the reference solution changes for newer versions of
dune-alugrid and one of the main purposes of the lens problem is to
allow comparison with Dumux relatively easily. (Dumux usese YaspGrid
for its version of the lens problem.)
- start with an initial "do nothing" episode of 100 days to get
hydrostatic conditions.
- after that, produce oil and inject water for 900 days. (thereafter
the reservoir will be empty.)
- make the problem work with element centered FV discretizations. this
requires to make the width of the injection/production areas at
least one cell wide. This is achieved by using the new "WellWidth"
property which specifies the with of wells as a factor of the total
domain width.
- make the problem work with fully compositional models. This implied
to calculate the full composition for the fluid states which specify
the initial condition and the thermodynamic state at the wells.
- add tests and reference solutions for any combination of the {ECFV,
VCFV} discretizations and the {black-oil, NCP} models.
- the residual now does not consider constraints anymore
- instead, the central place for constraints is the linearizer:
- it gets a constraintsMap() method which is analogous to residual()
but it stores (DOF index, constraints vector) pairs because
typically only very few DOFs need to be constraint.
- the newton method consults the linearizer's constraint map to update
the error and the current iterative solution. the primary variables
for constraint degrees of freedom are now directly copied from the
'Constraints' object to correctly handle pseudo primary variables.
- the abilility to specify partial constraints is removed, i.e., it is
no longer possible to constrain some equations/primary variables of
a degree of freedom without having to specify all of them. The
reason is that is AFAICS with partial constraint DOFs it is
impossible to specify the pseudo primary variables for models which
require them (PVS, black-oil).
because of this, the reference solution for the Navier-Stokes test
is updated. the test still oscillates like hell, but fixing this
would require to implement spatial discretizations that are either
better in general (e.g., DG methods) or adapted to Navier-Stokes
problems (e.g., staggered grid FV methods). since both of these are
currently quite low on my list of priorities, let's just accept the
osscillations for now.
* github.com:OPM/ewoms:
adaptation works, needs revision.
[dune-fem] using discrete function works.
some further work on grid adaptivity
dune.module: add dune-fem as a noptional dependency
Conflicts:
ewoms/common/start.hh
ewoms/io/basegridmanager.hh
ewoms/parallel/mpihelper.hh
this is not needed anymore because the grid manager is no longer a
singleton and the grid is thus is always destructed before
MPI_Finalize() is called.
i.e., removing redundant namespace open- and closings due to the fact
that the property system now resides in the 'Ewoms' namspace instead
of in 'Opm', and making the headercheck work for all headers.
now the generic part of the update of the solution vector is done in
the base class and the derived classes can chose to only do the update
of the primary variables of the individual DOFs.
This reverts commit c6c271f3ee. After a
more thorough investigation, the cannonical name of these quantities
turned out to be "* formation volume factor"...
... and use the parallel AMG solver for the CO2 injection problem.
this makes performance comparisions with Dumux much easier as the
solver performance should be more similar.
this helps to keep the core blackoil model code lean and mean and it
is also less confusing for newbies because the ECL blackoil simulator
is not a "test" anymore.
in case somebody wonders, "ebos" stands for "&eWoms &Black-&Oil
&Simulator". I picked this name because it is short, a syllable, has
not been taken by anything else (as far as I know) and "descriptive"
names are rare for programs anyway: everyone who does not yet know
about 'git' or 'emacs' and tells me that based on their names they
must be a source-code managment system and an editor gets a crate of
beer sponsored by me!
This code is required in the first place because opm-material always
specifies all parameters in terms of the wetting saturations while the
gas is the non-wetting phase in a gas-oil system.
this does not disrupt the block nature of the linearized matrix
(i.e. Dune::BCRSMatrix is still used), but if the number of auxiliary
equations is smaller than that of the "main" discretization, the
superfluous equations are padded. if the number of additional
equations are larger than that of the equation, additional DOFs are
added.
the biggest change is that it is now based on a new approach: the well
model now always calculates the bottom hole pressure for the full well
when asked for a source term. This change makes it possible to
implement cross flow within wells properly and should also make the
well model physically correct.
Also, the well model now uses the connection transmissibility factor
which makes it possible to use this quantity if it is specified by the
deck...
the goal is to make it faster on computers with many cores: The
easiest way to do this is to ensure that the longest running tests are
not taking too much time and that they need about the same time. Thus
this patch contains the following changes which limits the CPU time
taken by each test to about two minutes in debug mode on my machine:
- the water-air problem using the non-isothermal primary variable
switching model now uses an 16x16 instead of a 32x32 grid. as a
compensation it now runs for a year instead of 5000 seconds and the
global grid refinement is now tested.
- the end time of the lens problem ctests is now 3000 instead of
30000 seconds. The binary itself does not change at all.
- sort the tests in the CMakeLists.txt roughly in the order of their
required time. (this will cause ctest not having to wait for long
running test which were started late for too long.)
it was used for debugging intersection mappers. to make this include
work, dune-cornerpoint must be available and that the intersection
mapper PR must be merged.
this means that all code which could potentially throw an exception is
moved to this method(). (In particular FluidSystem::init() proved
troublesome in the past.) Besides avoiding segmentation the faults
which stem from exceptions thrown in constructors, this also has the
advantage that simulations which spend a noticable amount of time to
initialize stop at the "correct" place, i.e. after the "Finish init of
the problem" message was printed by the simulator...
this regressed after time step index of the initial solution was
changed from 0 (actually, this was also 0 for the first time step...)
to -1 in b30af664.
this method checks that the difference in the storage terms before and
after a time step is the same as the accumulated fluxes over the
domain boundary plus the source terms.
... and actually use it for the lens problems. This seems to have been
disabled for debugging and later it was probably forgotten to turn it
on again. This led to some minor bit-rot in that code...
The reason for this is to be able to modify the tolerance according to
grid size: The NewtonTolerance parameter has been renamed to
NewtonRawTolerance and for the porous media models is divided by the
square root of the volume of the smallst finite volume in the grid to
get the final tolerance for the Newton method. This is necessary
because very large grids need to achive a higher volumetric accuracy
in the residual than very small ones...
basically the init() method was split into a finishInit() method which
fills the data structures allocated in the constructor with meaningful
data and into applyInitialSolution() which does just that (and no
more!)
"intensive" means that the value of these quantities at a given
spatial location does not depend on any value of the neighboring
intensive quantities. In contrast, "extensive" quantities depend in
the intensive quantities of the environment of the spatial location.
this change is necessary is because the previous nomenclature was very
specific to finite volume discretizations, but the models themselves
were already rather generic. (i.e., "volume variables" are the
intensive quantities of finite volume methods and "flux variables"
are the extensive ones.)
because "manager" sounds less religious than "creator" and the
GridCreators did all kinds of other stuff besides creating the grid.
this patch also gets rid of the static function inside these classes,
which should make them easier to understand...
this also comes with moving responsibilities around and some smaller
cleanups for the grid creation. (although grid creation could be
possibly done by the simulator now, the GridCreator concept has not
been abandoned, yet...)
this allows to retrieve the name of the problem before it is
instantiated. this is required to be able to print the "Initializing
problem" message at the correct point (i.e., before instantiating the
problem).
and some other minor changes. (if you need line search the issue is
probably caused a different problem and line search would be just a
work-around anyway.)
