- 03 Jan, 2023 2 commits
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Martin Utz authored
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Martin Utz authored
Add pure bedload model See merge request !138
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- 21 Dec, 2022 2 commits
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Martin Utz authored
The number of the shallowwater equations was hard coded to 3, which caused a problem within the pure bedload model. Now the number of shallowwater equations is got by ModelTraits::numSweEq().
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Martin Utz authored
This is a multigrain model, which does not include the shallow water equations.
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- 02 Dec, 2022 3 commits
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Martin Utz authored
Add hiding and exposure See merge request !137
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Martin Utz authored
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Martin Utz authored
The segmentation fault occured if the number of grain classes was smaller than the maximum number of grain classes. The problem was, that in the spatial params the vector bedloadformula_ is only initialized for the actuelly existing grain classes, but in the volvars it was looped over this vector by the maximum number of grain classes. This bug was introduced in commit 73668576.
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- 01 Dec, 2022 1 commit
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Martin Utz authored
The provision of output variables should not part of the layer model. Instead it should be added in the problem.
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- 15 Nov, 2022 2 commits
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Martin Utz authored
improve secondary currents again See merge request !136
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Martin Utz authored
This just consequent, since the bed shear stress is modified in the presence of secondar currents. The velocity, which is also used within the slope effect has already be modified.
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- 14 Nov, 2022 1 commit
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Martin Utz authored
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- 11 Nov, 2022 4 commits
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Martin Utz authored
Improve secondary currents Closes #81 See merge request !135
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Martin Utz authored
The modified velocity is used for the slope effect as well as for the riemann solver
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Martin Utz authored
Up to now the bed shear stress was rotated by the secondary currents angle, which is not correct, since the secondary currents add an additional component to the bed shear stress.
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Martin Utz authored
The direction change due to the secondary currents is now applied within the bedload transport, since we can use it here to modify the bed shear stress, as it should be. Up to now it was applied to the bedlaod discharge, what was not correct. Since the bed shear stress does not occure in the Grass bedload transport formula we apply the direction change to the velocity.
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- 08 Nov, 2022 1 commit
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Martin Utz authored
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- 28 Oct, 2022 3 commits
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Martin Utz authored
Improve assemble See merge request !134
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Martin Utz authored
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Martin Utz authored
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- 11 Oct, 2022 1 commit
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Martin Utz authored
Fix some bugs in the initialisation of the hirano layer model See merge request !133
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- 07 Oct, 2022 3 commits
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Martin Utz authored
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Martin Utz authored
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Martin Utz authored
Use an eps to ensure that layer 1 vanishes during the initialisation of the Hirano layer model if it has the active layer thickness.
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- 06 Oct, 2022 1 commit
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Martin Utz authored
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- 05 Oct, 2022 1 commit
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Martin Utz authored
upperBoundaryLayer* -> upperLimitLayer*
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- 10 Aug, 2022 2 commits
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Martin Utz authored
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Martin Utz authored
Before it was 1e-6 m now it is 1e-3 m.
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- 09 Aug, 2022 4 commits
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Martin Utz authored
[limiting] Use LET limiter instead of linear limiting See merge request !132
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Martin Utz authored
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Martin Utz authored
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Martin Utz authored
The LET limiter has more posibilities to influence the limiting.
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- 04 Aug, 2022 2 commits
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Martin Utz authored
Fix limiting bedload discharge flux See merge request !131
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Martin Utz authored
The previous default values don't work for river models. Therefore they werde removed.
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- 03 Aug, 2022 3 commits
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Martin Utz authored
The bounds for the limiting of the bedload discharge are dependent of the massFraction of the corresonding grain class. This caused negative sediment masses, since the bounds for the limiting became small for small mass fractions. To avoid this we introduced minimal bounds for the limiting, which depend on the representative grain diameter.
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Martin Utz authored
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Martin Utz authored
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- 27 Jul, 2022 4 commits
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Martin Utz authored
Resolve "Use only the bottom shear stress of the friction law" Closes #79 See merge request !130
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Martin Utz authored
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Martin Utz authored
This commit causes changes in the result, since the bottom shear stress provided by the friction law differs since: * Up to know only Manning with a spatially constant friction parameter was used Now the actuall bottom shear stress from the HN simulation is used. * Also whenn using Mannings law the friction law calculates the bottom shear stress differently.
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Martin Utz authored
This avoids a division by zero, which causes NaN values.
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