- Sep 07, 2024
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Sander, Oliver authored
Instead, use LocalIntegralEnergy and the newly introduced densities for bulk models or planar shell models. While doing so, give an error message when non-trivial volume loads are requested. I have no example file that actually uses them at the moment, and just by looking at the code I find it hard to believe that they actually worked. Getting them to work will mean having introduce a density for volume loads, which don't want to do until I need them. Since this is the last use of the CosseratEnergyLocalStiffness class, this patch remove the entire class as well.
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- Aug 30, 2024
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Sander, Oliver authored
That way, we can also set the initial microrotation -- previously it was hard-wired to the identity matrix. Being able to explicitly choose the initial microrotation allows to start, in particular, from a twisted strip.
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- Aug 22, 2024
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Sander, Oliver authored
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Sander, Oliver authored
Previously, the method basically hand-implemented a writer for VTK files. Using dune-vtk instead leads to much shorter and simpler code, and gives us access to all the dune-vtk niceties, like binary files and high-order grid cells.
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- Aug 21, 2024
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Sander, Oliver authored
Rather than the grid itself. Because the grid view is all that a writer needs to know about.
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Sander, Oliver authored
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Sander, Oliver authored
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- Aug 12, 2024
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Sander, Oliver authored
That way, a single Python file is enough to describe the entire boundary value problem.
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Sander, Oliver authored
Rather than as our homegrown .parset. That way, after more changes this will allow to have the entire problem description in a single file, including the boundary data.
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Sander, Oliver authored
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- Jul 06, 2024
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Sander, Oliver authored
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- May 01, 2024
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Sander, Oliver authored
They were expected to be the factors of a ProductManifold which is also a template parameter. Expecting the product and the factors is redundant. We simply extract the factors from the product now.
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- Apr 30, 2024
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Sander, Oliver authored
Previously, it expected two factor spaces, as separate template parameters. Taking a single ProductManifold type is more consistent with GeodesicFEAssembler, and it allows to eventually generalize the code to more factors, if desired.
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Sander, Oliver authored
... but disallow a plain pointer. This increases consistency with the GeodesicFEAssembler class.
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- Apr 20, 2024
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Sander, Oliver authored
dune-elasticity also has densities, but they implement a slightly different interface. Instead of having special code for such densities in the LocalIntegralAssembler, add a wrapper that makes densities from dune-elasticity look like dune-gfe densities.
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- Mar 25, 2024
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Sander, Oliver authored
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- Mar 24, 2024
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Sander, Oliver authored
There is no need to wrap the std::function that stores the Neumann force density into a std::shared_ptr.
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Sander, Oliver authored
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- Mar 19, 2024
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Sander, Oliver authored
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Sander, Oliver authored
Plus some minor cleanup
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Sander, Oliver authored
This replaces the dedicated implementation of the quadrature loop for harmonic energies -- that is not needed anymore. In particular this means that the test for it can be removed. In theory it should be replaced with a test for the harmonic energy *density*, but that density implementation is so short that it doesn't really require a separate test.
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Sander, Oliver authored
Rather than using preprocessor switches. That's too fragile and not extensible.
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Sander, Oliver authored
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Sander, Oliver authored
If the target manifold is a product space, then ProductManifold must be used, and not a variadic list of the factor space types.
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- Feb 12, 2024
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Sander, Oliver authored
They do the same thing, essentially.
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- Feb 07, 2024
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Sander, Oliver authored
This is what the non-mixed ADOL-C assembler does, and I want to merge the two.
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Sander, Oliver authored
The new method is Fufem::markBoundaryPatchDofs, which apparently works in just the same way.
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- Jan 15, 2024
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Sander, Oliver authored
The ProductManifold class generalizes RigidBodyMotion, and can do everything that the RigidBodyMotion class can. Therefore there is no point in keeping RigidBodyMotion any longer. Having two implementations for the same thing will just confuse people.
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- Jan 08, 2024
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Sander, Oliver authored
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- Jan 05, 2024
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Sander, Oliver authored
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- Oct 27, 2023
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Lisa Julia Nebel authored
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- May 24, 2023
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Sander, Oliver authored
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- May 22, 2023
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Sander, Oliver authored
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Sander, Oliver authored
It was apparently not used. If you should ever need something like this in the future, please use periodicbasis.hh from dune-functions.
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- May 16, 2023
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Sander, Oliver authored
The old style has been deprecated for a long time, and is not supported by dune-fufem anymore. (In particular, the code discretizationerror.hh now requires functions to satisfy the dune-functions function interface.) In the wake of this, compute-disc-error.cc gets a number of changes. Let's hope I didn't screw up anything.
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Sander, Oliver authored
There are two important changes: First of all, the new class implements the `dune-functions` interface rather than the deprecated one based on inheritance from `VirtualGridViewFunction`. Secondly, the new class does not hard-wire geodesic interpolation anymore. Rather, you can give it interpolation classes which then govern how interpolation is done. This change was long overdue. It was now needed to make gradient-flow.cc compile with the post 2.9 version of dune-fufem again.
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Sander, Oliver authored
The code erroneously used std::tie to combine two local variables to a single return value. That may fail because std::tie produces a tuple of references. Once the method has returned these references may or may not be valid anymore. I am surprised that this bug has not caused trouble much earlier.
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- Apr 24, 2023
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
In particular: - Use the CosseratVTKWriter also for MIXED_SPACE = 1, only print out the deformation though - Use a SubsamplingVTKWriter only for dim==gridDim==3
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