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…nchmark Update spiegelman newton benchmark
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benchmarks/newton_solver_benchmark_set/spiegelman_et_al_2016/README.md
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# Newton Solver Benchmark Set - Spiegelman et at. (2016) | ||
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The files in [this directory](https://github.com/geodynamics/aspect/tree/main/benchmarks/newton_solver_benchmark_set/spiegelman_et_al_2016) | ||
can be used to recreate the Spiegelman et al. (2016) flow figures from | ||
{cite:t}`fraters:etal:2019`. Adjust both the `metabash.sh` and `bash.sh` files to | ||
reflect the parameter search you are interested in and run the metabash script. | ||
If you have run exactly the same runs as shown in the paper, you can use the | ||
`cp_P-minLT-res-it-vel_BV.sh` script to recreate the figures in that paper. | ||
This script requires that the drucker prager compositions plugin is installed. | ||
It should be possible to replicate the same behavior with the visco plastic | ||
plugin. | ||
can be used to recreate the figures from | ||
{cite:t}`fraters:etal:2019` reproducing the {cite:t}`spiegelman:etal:2016` benchmark. | ||
`input.prm` is the setup of one of the benchmark | ||
models and `run.sh` will execute a series of model runs. Before you can execute | ||
the benchmark you will have to compile the plugin `drucker_prager_compositions.cc` in | ||
the same directory, the process of compiling plugins is described in [](sec:benchmark-run). | ||
After you have executed `run.sh`, you can use the gnuplot plotting script | ||
`plot.gnuplot` to recreate Fig. 4 of {cite:t}`fraters:etal:2019`. | ||
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```{figure-md} fig:benchmark-newton-spiegelman-2016 | ||
<img src="doc/figure_4.png" /> | ||
Convergence history of several models of the Spiegelman et al. benchmark: a reproduction of three of the nine pressure dependent Drucker–Prager cases with a resolution of 64 × 16 cells. Top: results for computations where linear systems are solved with a maximum relative tolerance of 0.9. Bottom: The same models solved with a tolerance of $10^{-8}$. The initial Picard iteration is always solved to a linear tolerance of $10^{-14}$. Left to right: different prescribed velocities of u0 = 2.5, 5, and 12.5 cm\yr, and different background reference viscosities of respectively $\eta_{ref}$ = $10^{23}$, $10^{24}$ and $10^{25}$ Pa s. Horizontal axis: number of the non-linear (outer) iteration; and vertical axis: non-linear residual. "DC Picard" refers to a defect correction Picard iteration, see the paper describing this solver. | ||
``` | ||
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The nonlinear convergence behavior of ASPECT's different nonlinear solvers is shown in {numref}`fig:benchmark-newton-spiegelman-2016`. |
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benchmarks/newton_solver_benchmark_set/spiegelman_et_al_2016/auto_logs/.gitignore
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benchmarks/newton_solver_benchmark_set/spiegelman_et_al_2016/bash.sh
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benchmarks/newton_solver_benchmark_set/spiegelman_et_al_2016/bash_autos/.gitignore
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