- Jan 11, 2021
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Timo Koch authored
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- Oct 30, 2020
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- Oct 28, 2020
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Mathis Kelm authored
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- Oct 27, 2020
- Oct 16, 2020
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- Sep 30, 2020
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Kilian Weishaupt authored
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- Sep 29, 2020
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* Loads in solution from rans2c for a rans2cni test * Tests rans2cni faster, plus loading a partial solution for ICs
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Kilian Weishaupt authored
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- Sep 09, 2020
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Timo Koch authored
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- Aug 27, 2020
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- Aug 06, 2020
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Dennis Gläser authored
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- Jun 15, 2020
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Timo Koch authored
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- May 04, 2020
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Dennis Gläser authored
This commit also modifies the tracer_tracer test, as this failed for box after removing the elembctypes. This is because it was using Neumann no-flow boundary conditions for the fracture domain on the left boundary while the bulk problem used Dirichlet BCs. The old elembctypes for box were discarding Dirichlet BCs on those nodes on the boundary that also couple to fractures in order for the coupling conditions to be fulfilled. However, that discards the boundary condition. With this commit, Dirichlet BCs are always fulfilled, but for the tracer test this means that as a consequence, the pressure in the fracture on the left side is equal to the bulk pressure - because it uses Dirichlet-type coupling conditions. This commit changes the test such that it uses Dirichlet BCs in the bulk domain only on the lower part of the boundary such that the fracture touches the domain boundary at a no-flow boundary.
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- Apr 28, 2020
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Ned Coltman authored
* Reduced inital dt * Fixed timesteps * Adapted the reference solution
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- Apr 27, 2020
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with contributions by Felix Weinhardt and some proof reading by Timo Koch and Dennis Gläser
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- Apr 23, 2020
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Bernd Flemisch authored
The distribution of an unstructured across several processes is not stable in the sense that a process will always get the same elements. Not over several Dune versions and possibly even not between different machines. Threfore, don't compare the solution for a single process.
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- Apr 22, 2020
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[test][2pncminni] increase runtime to test precipitation, use fixed time-step size increment, adapt reference
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- Apr 16, 2020
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- Apr 07, 2020
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- Apr 06, 2020
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Timo Koch authored
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- Mar 31, 2020
- Mar 30, 2020
- Mar 26, 2020
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The idea of the tracer model is really tied to Fickian diffusion and components with small concentration diffusing in a bulk phase. Hence also it's name. The Maxwell-Stefan test actual models 3 gaseous components where none of the components is really the main phase but most importantly there is no bulk phase with a main component that is not considered in the equations. Thus the 1pnc model is the right choice for such a test. This changes the test to derive from the 1pnc model. As for the given setting with only Neumann boundaries the 1pnc wouldn't convergence for a compressible fluid, the Ideal gas law is used to model a compressible gas. The same test actually exists for the 1pnc model already in 1pnc/implicit/1p3c. Thus this commit simply removes the tracer test.
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- Mar 18, 2020
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Timo Koch authored
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- Mar 17, 2020
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with changes over processor boundaries adapt other tests to match new injection rate, harmonize timesteps with lower DtInitial and MaxTimeStepSize
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stationary, outflow at outlet, block profile at inlet.
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Actually use the surface grid. Update references.
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- Mar 15, 2020
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Timo Koch authored
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- Mar 04, 2020
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Martin Schneider authored
the correct state initialization in the Newton method results in a new solution
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- Feb 01, 2020
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Timo Koch authored
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