- Jul 09, 2021
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Lisa Julia Nebel authored
WHITESAPCES for previous commit: Add the option to use the Riemannian Proximal Newton solver also for problems with dim = dimwold
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
Use cholmod if the dune-solvers version >= 2.8, use umfpack for older versions
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Lisa Julia Nebel authored
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- Jun 10, 2021
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
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- May 05, 2021
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Lisa Julia Nebel authored
Change the keywords for switching between the solvers to trustRegion and proximalNewton also in film-on-substrate
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Lisa Julia Nebel authored
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- Apr 22, 2021
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Lisa Julia Nebel authored
Now all combinations of dim = dimworld or dim != dimworld and MIXED_SPACE = 0 or MIXED_SPACE = 1 at least compile.
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Lisa Julia Nebel authored
This has to be dimworld and not dim.
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
The StressFreeStateGridFunction is the actual parametrization from the grid to the nonplanar Cosserat shell in stress-free state. The geometries of the StressFreeStateGridFunction will then be used for all calculations instead of the linear geometries of the piecewise linear grid.
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Lisa Julia Nebel authored
This has been changed to Dune::Vtk::FormatTypes::ASCII in the dune-vtk module
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- Feb 16, 2021
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Sander, Oliver authored
The previous implementation worked only for first-order finite element spaces, because it assumed that grid vertices and Lagrange nodes were identical.
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- Feb 08, 2021
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Lisa Julia Nebel authored
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- Jan 20, 2021
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
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- Jan 19, 2021
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- Nov 20, 2020
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Sander, Oliver authored
So far, the Cosserat rod energy implementation hat a first-order finite element space hardcoded. This patch removes that restriction. As for the other models in this Dune module, the finite element basis is now a template parameter of the model energy, and can be set to any reasonable basis.
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Sander, Oliver authored
It is not a 'stiffness' anymore, but really only implements the energy.
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Sander, Oliver authored
This is a prerequisite to a) support for higher-order FE, and b) getting rid of the hand-written CosseratVTKWriter.
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Sander, Oliver authored
Previously, the rod3d code used a hand-implemented first derivative of the rod energy, and FD for the second derivatives. This patch replaces this by ADOL-C for both first and second derivatives. Advantages are: * The code is much shorter, and easier to understand. * The previous code contained interpolation formulae for first-order 1d geodesic finite elements. This restricted rod problems to first-order GFE. A follow-up patch will allow higher-order approximations. * The new code runs roughly twice as fast.
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Sander, Oliver authored
GeodesicFEAssembler can replace it without problems.
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- Nov 08, 2020
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Sander, Oliver authored
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Sander, Oliver authored
In the 'mixed' case the volume term was simply forgotten, and not actually handed to the assembler.
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Sander, Oliver authored
It is very unlikely that somebody will use that ever again.
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Sander, Oliver authored
Rather than using a default file, which was the case previously.
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Sander, Oliver authored
Otherwise the program aborts for the usual mysterious reasons.
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Sander, Oliver authored
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- Nov 05, 2020
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
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Lisa Julia Nebel authored
When dune-curvedgeometry is not found, the normal Derivative is set to zero.
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Sander, Oliver authored
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- Oct 28, 2020
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Lisa Julia Nebel authored
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- Oct 21, 2020
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Lisa Julia Nebel authored
Use GFE::LocalEnergy, GFE::LocalIntegralEnergy, GFE::SumEnergy (and delete GFE::SumCosseratEnergy).
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- Oct 12, 2020
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Lisa Julia Nebel authored
film-on-substrate uses a class of dune-elasticity that is not available in earlier versions
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- Oct 06, 2020
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Lisa Julia Nebel authored
Virtual Function is deprecated after dune 2.7.
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