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| ALLOW_GPU_PRINTF | ||
| AMREX_DEBUG | ||
| AMREX_PARTICLES | ||
| AMREX_SPACEDIM | ||
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132 changes: 66 additions & 66 deletions
132
Exec/science/Detonation/ci-benchmarks/sdc_det_plt00040_extrema.out
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| # Shock Burning Experiments | ||
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| This directory is meant to explore shock burning with detonation. Compile as: | ||
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| ``` | ||
| make USE_SIMPLIFIED_SDC=TRUE USE_SHOCK_VAR=TRUE NETWORK_DIR=aprox13 -j 4 | ||
| ``` | ||
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| Then the script `setup_runs.py` will setup a suite of simulations with | ||
| the following resolutions into separate directories (using the | ||
| `inputs-shock-burn.template`): | ||
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| | resolution | base grid | levels (4x jumps) | | ||
| | ------------ | ----------- | ------------------- | | ||
| | 24 km | 48 | 1 | | ||
| | 12 km | 96 | 1 | | ||
| | 6 km | 192 | 1 | | ||
| | 3 km | 384 | 1 | | ||
| | 1.5 km | 768 | 1 | | ||
| | 0.1875 km | 6144 | 1 | | ||
| | 2343.74 cm | 12288 | 2 | | ||
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| you can set the value of the shock detection threshold there | ||
| and the directory names will reflect that setting. | ||
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| ## plotting | ||
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| The following scripts can make useful plots (some use the | ||
| `detonation.py` module as support): | ||
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| * `det_speed_comp.py` : plot detonation speed vs. resolution, using | ||
| simple differencing to estimate the detonation speed from the last 3 | ||
| plotfiles. | ||
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| * `profile_compare.py` : given a list of pruns (from different | ||
| resolutions), make a plot showing all of their profiles together. | ||
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| * `profiles.py` : for a single run, plot profiles of T and enuc for | ||
| several times. | ||
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| * `show_shock_flag.py` : simply plot the shock variable on top of T | ||
| and enuc profiles. | ||
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| * `zoom_summary.py` : given a list of runs (from different | ||
| resolutions), plot the last plotfile from each run, zoomed in on | ||
| where the peak energy generation is. |
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| #!/usr/bin/env python | ||
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| import matplotlib.pyplot as plt | ||
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| import detonation | ||
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| runs = [("res24.0km", 24), | ||
| ("res12.0km", 12), | ||
| ("res6.0km", 6), | ||
| ("res3.0km", 3), | ||
| ("res1.5km", 1.5), | ||
| ("res0.1875km", 0.1875)] #, | ||
| #("res0.024km", 0.024)] #, | ||
| #("res0.003km", 0.003)] | ||
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| nsb1_runs = [("res24.0km_noshockburn_1", 24), | ||
| ("res12.0km_noshockburn_1", 12), | ||
| ("res6.0km_noshockburn_1", 6), | ||
| ("res3.0km_noshockburn_1", 3), | ||
| ("res1.5km_noshockburn_1", 1.5), | ||
| ("res0.1875km_noshockburn_1", 0.1875)] #, | ||
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| nsb23_runs = [("res24.0km_noshockburn_0.666", 24), | ||
| ("res12.0km_noshockburn_0.666", 12), | ||
| ("res6.0km_noshockburn_0.666", 6), | ||
| ("res3.0km_noshockburn_0.666", 3), | ||
| ("res1.5km_noshockburn_0.666", 1.5), | ||
| ("res0.1875km_noshockburn_0.666", 0.1875)] #, | ||
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| res = [] | ||
| v = [] | ||
| dv = [] | ||
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| for ddir, dx in runs: | ||
| res.append(dx) | ||
| d = detonation.Detonation(ddir) | ||
| v.append(d.v) | ||
| dv.append(d.v_sigma) | ||
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| nsb23_res = [] | ||
| nsb23_v = [] | ||
| nsb23_dv = [] | ||
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| for ddir, dx in nsb23_runs: | ||
| nsb23_res.append(dx) | ||
| d = detonation.Detonation(ddir) | ||
| nsb23_v.append(d.v) | ||
| nsb23_dv.append(d.v_sigma) | ||
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| nsb1_res = [] | ||
| nsb1_v = [] | ||
| nsb1_dv = [] | ||
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| for ddir, dx in nsb1_runs: | ||
| nsb1_res.append(dx) | ||
| d = detonation.Detonation(ddir) | ||
| nsb1_v.append(d.v) | ||
| nsb1_dv.append(d.v_sigma) | ||
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| fig, ax = plt.subplots() | ||
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| ax.errorbar(res, v, yerr=dv, fmt="o", label="burning in shocks allowed") | ||
| ax.errorbar(nsb23_res, nsb23_v, yerr=nsb23_dv, fmt="d", label="no shock burning (f=2/3)") | ||
| ax.errorbar(nsb1_res, nsb1_v, yerr=nsb1_dv, fmt="d", label="no shock burning (f=1)") | ||
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| ax.set_xlabel(r"$\Delta x$ (km)") | ||
| ax.set_ylabel(r"$v_\mathrm{det}$ (cm / s)") | ||
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| ax.legend() | ||
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| ax.set_xscale("log") | ||
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| fig.savefig("det_speeds.png") |
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