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Partitioned Pipe Multiscale Tutorial
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| - Added a new Partitioned Pipe Multiscale tutorial including 1D–3D, 3D–1D, 1D–1D, and 3D–3D coupling configurations using OpenFOAM and Nutils [#677](https://github.com/precice/tutorials/pull/677) |
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| --- | ||
| title: Partitioned Pipe — Geometric Axial Multiscale | ||
| keywords: OpenFOAM, Nutils, preCICE, geometric multiscale, fluid | ||
| summary: The Partitioned Pipe — Geometric Axial Multiscale tutorial couples a 1D pipe model with a 3D CFD pipe using preCICE. | ||
| --- | ||
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| {% note %} | ||
| Get the [case files of this tutorial](https://github.com/precice/tutorials/tree/develop/partitioned-pipe-multiscale), as continuously rendered here, or see the [latest released version](https://github.com/precice/tutorials/tree/master/partitioned-pipe-multiscale) (if there is already one). Read how in the [tutorials introduction](https://precice.org/tutorials.html). | ||
| {% endnote %} | ||
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| ## Setup | ||
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| We solve a simple **partitioned pipe problem** using a 1D–3D coupling approach. | ||
| In this tutorial, the computational domain is split into two coupled regions: a 1D pipe section and a 3D pipe section. | ||
| The coupling is performed using **preCICE**. | ||
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| In addition to the 1D–3D setup, this tutorial also includes configurations for **1D–1D** and **3D–3D** coupling. | ||
| These variants can be beneficial for validation studies, solver comparisons, or for investigating the influence of model dimensionality. | ||
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| In the following, $\mathrm{1D}$ denotes the reduced-order domain (e.g., a Nutils solver) and $\mathrm{3D}$ denotes the full 3D CFD domain (e.g., OpenFOAM). | ||
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| The problem consists of a straight pipe of length $L = 40 \mathrm{m}$ and diameter $D = 10 \mathrm{m}$. We partition the domain at $z_c = 20 \mathrm{m}$, where the coupling interface is located. The pipe axis is aligned with the z-axis. | ||
| The **1D domain** solves the flow equations using Nutils, while the **3D domain** is solved using OpenFOAM. | ||
| Both solvers are coupled via preCICE by exchanging the **pressure** and **axial velocity** at the interface. | ||
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| Two coupling directions are possible: | ||
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| - **1D → 3D**: The 1D solver provides the interface velocity to the 3D solver, which responds with pressure. | ||
| - **3D → 1D**: The 3D solver provides the velocity, and the 1D solver returns the pressure. | ||
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| The global outlet (end of the rightmost domain) is set to $p_{\mathrm{out}} = 0 \mathrm{Pa}$. | ||
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| For the **3D → 1D** coupling, the 3D inlet velocity is prescribed as a **parabolic (Poiseuille)** profile with a bulk velocity of $u_{\mathrm{in}} = 0.1 \mathrm{m/s}$ | ||
| implemented using a `codedFixedValue` boundary condition. This ensures a physically realistic velocity distribution consistent with the 1D model. | ||
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| For the **1D → 3D** coupling, the inlet velocity is set to $u_{\mathrm{in}} = 0.1 \mathrm{m/s}$. | ||
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| ## Configuration | ||
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| preCICE configuration for the 1D-3D simulation (image generated using the [precice-config-visualizer](https://precice.org/tooling-config-visualization.html)): | ||
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|  | ||
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| preCICE configuration for the 3D-1D simulation: | ||
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|  | ||
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| ## Available solvers | ||
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| - OpenFOAM (**pimpleFoam**). An incompressible/transient OpenFOAM solver. See the [OpenFOAM adapter documentation](https://precice.org/adapter-openfoam-overview.html). | ||
| - Nutils. A Python-based finite element framework. For more information, see the [Nutils adapter documentation](https://precice.org/adapter-nutils.html) | ||
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| ## Running the Simulation | ||
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| First, select which coupling you want to run. This sets the correct `precice-config.xml` symlink (by default, set to `1d3d`): | ||
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| ```bash | ||
| # Choose one configuration | ||
| ./setcase.sh 1d3d | ||
| # or | ||
| ./setcase.sh 3d1d | ||
| # or | ||
| ./setcase.sh 1d1d | ||
| # or | ||
| ./setcase.sh 3d3d | ||
| ``` | ||
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| Open **two terminals** and start the corresponding participants for your chosen setup. | ||
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| ### Example A — 1D → 3D coupling | ||
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| Terminal 1: | ||
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| ```bash | ||
| cd fluid1d-left-nutils | ||
| ./run.sh | ||
| ``` | ||
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| Terminal 2: | ||
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| ```bash | ||
| cd fluid3d-right-openfoam | ||
| ./run.sh | ||
| ``` | ||
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| ### Example B — 3D → 1D coupling | ||
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| Run `./setcase.sh 3d1d` and then navigate to the respective directories. | ||
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| Terminal 1: | ||
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| ```bash | ||
| cd fluid3d-left-openfoam | ||
| ./run.sh | ||
| ``` | ||
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| Terminal 2: | ||
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| ```bash | ||
| cd fluid1d-right-nutils | ||
| ./run.sh | ||
| ``` | ||
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| ## Visualization | ||
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| The output of the coupled simulation is written into the folders `fluid1d-left-nutils`, `fluid1d-right-nutils`, `fluid3d-left-openfoam`, and `fluid3d-right-openfoam`, depending on which coupling direction (`1d3d` or `3d1d`) you selected. | ||
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| ### 3D domain (OpenFOAM) | ||
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| For the 3D participant, all simulation results are stored in the time directories inside the respective case folder (e.g., `fluid3d-right-openfoam/`). | ||
| You can visualize the flow field and pressure distribution using **ParaView** by opening the case file: | ||
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| ```bash | ||
| paraview fluid3d-right-openfoam/fluid3d-right-openfoam.foam | ||
| ``` | ||
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| or, for the left domain if applicable: | ||
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| ```bash | ||
| paraview fluid3d-left-openfoam/fluid3d-left-openfoam.foam | ||
| ``` | ||
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| Typical fields to inspect include: | ||
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| - `p` – pressure | ||
| - `U` – velocity | ||
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| We also record pressure and velocity at fixed points each time step using the OpenFOAM `probes` function object. | ||
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| **Probe setup (excerpt):** | ||
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| ```c | ||
| #includeEtc "caseDicts/postProcessing/probes/probes.cfg" | ||
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| fields (p U); | ||
| probeLocations | ||
| ( | ||
| (0 0 20) | ||
| (0 0 40) | ||
| ); | ||
| // For the left 3D domain use instead: | ||
| // probeLocations ((0 0 0) (0 0 20)); | ||
| ``` | ||
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| **Output location:** | ||
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| - `fluid3d-right-openfoam/postProcessing/probes/0/p` | ||
| - `fluid3d-right-openfoam/postProcessing/probes/0/U` | ||
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| In addition to point probes, the 3D participant samples the **axial pressure distribution** along the pipe centerline using `sampleDict`. This provides the spatial pressure variation along the pipe and allows direct comparison with the 1D solution at the latest time step. | ||
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| The tutorial includes a `sampleDict` in the 3D cases: | ||
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| - `fluid3d-left-openfoam/system/sampleDict` | ||
| - `fluid3d-right-openfoam/system/sampleDict` | ||
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| **sampleDict (excerpt):** | ||
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| ```cpp | ||
| FoamFile | ||
| { | ||
| version 2.0; | ||
| format ascii; | ||
| class dictionary; | ||
| location "system"; | ||
| object sampleDict; | ||
| } | ||
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| type sets; | ||
| libs ("libsampling.so"); | ||
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| setFormat raw; | ||
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| sets | ||
| ( | ||
| centerline | ||
| { | ||
| type uniform; | ||
| axis z; | ||
| start (0 0 0); | ||
| end (0 0 20); | ||
| nPoints 200; | ||
| } | ||
| ); | ||
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| fields (p); | ||
| ``` | ||
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| The sampling is executed automatically during the run. | ||
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| **Output location:** | ||
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| ```text | ||
| postProcessing/sampleDict/<latestTime>/centerline_p.xy | ||
| ``` | ||
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| The file contains two columns: | ||
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| 1. axial coordinate `z` | ||
| 2. pressure `p` | ||
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| ### 1D domain (Nutils) | ||
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| The 1D solver writes a `probes.txt` with semicolon-separated time series: | ||
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| ```text | ||
| time; p_in; u_in; p_out; u_out; p_mid; u_mid | ||
| ``` | ||
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| where: | ||
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| - `p_in`, `u_in` → pressure and velocity at the inlet of the 1D domain | ||
| - `p_out`, `u_out` → pressure and velocity at the outlet of the 1D domain | ||
| - `p_mid`, `u_mid` → pressure and velocity at the midpoint of the 1D domain | ||
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| The 1D solver also writes a `final_fields.txt` with space-separated values: | ||
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| ```text | ||
| x u p | ||
| ``` | ||
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| They correspond to the axial position, velocity and pressure at the last time-step, i.e., at $t = 5 \mathrm{s}$. | ||
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| ### Plotting axial pressure distribution (optional) | ||
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| To reproduce the axial pressure distribution shown in the figure below, a helper script is provided: | ||
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| ```bash | ||
| python plot-pressure-distribution.py | ||
| ``` | ||
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| By default, the script uses the `1d3d` case. | ||
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| You can also specify the coupling configuration explicitly: | ||
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| ```bash | ||
| python plot-pressure-distribution.py 1d3d | ||
| ``` | ||
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| ```bash | ||
| python plot-pressure-distribution.py 3d1d | ||
| ``` | ||
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| ```bash | ||
| python plot-pressure-distribution.py 1d1d | ||
| ``` | ||
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| ```bash | ||
| python plot-pressure-distribution.py 3d3d | ||
| ``` | ||
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| Allowed cases are: | ||
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| - `1d3d` | ||
| - `3d1d` | ||
| - `1d1d` | ||
| - `3d3d` | ||
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| Depending on the selected case, the script reads: | ||
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| - `final_fields.txt` from the 1D Nutils solver | ||
| - `centerline_p.xy` from the 3D OpenFOAM participant | ||
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| and combines both datasets to plot the pressure distribution along the coupled pipe. | ||
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| By default, the figures are saved to: | ||
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| ```text | ||
| images/pressure_distribution_<case>.png | ||
| ``` | ||
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| ### Example visualization | ||
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|  | ||
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| **Pressure along the pipe centerline.** The pressure decreases nearly linearly from **≈12.8 Pa** at the 3D inlet to **0 Pa** at the 1D outlet, consistent with steady, laminar Poiseuille flow. The 3D (0–20 m) and 1D (20–40 m) sections connect smoothly at the coupling interface. | ||
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|  | ||
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| **Parabolic velocity profile at the 3D outlet / coupling interface (z = 20 m).** | ||
| The profile is Poiseuille-like with a bulk velocity of **0.1 m/s**; consequently the **centerline velocity is ≈ 0.2 m/s** (≈ 2 × bulk) and vanishes at the wall (no-slip). This is the velocity state at the interface used for coupling to the 1D domain. | ||
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| #!/usr/bin/env sh | ||
| set -e -u | ||
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| # shellcheck disable=SC1091 | ||
| . ../tools/cleaning-tools.sh | ||
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| clean_tutorial . | ||
| clean_precice_logs . | ||
| rm -fv ./*.log | ||
| rm -fv ./*.vtu | ||
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|
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| probes.txt | ||
| final_fields.txt |
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| @@ -0,0 +1,10 @@ | ||
| #!/usr/bin/env sh | ||
| set -e -u | ||
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| . ../../tools/cleaning-tools.sh | ||
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| rm -f ./results/Fluid1D_* | ||
| rm -f ./probes.txt | ||
| rm -f ./final_fields.txt | ||
| clean_precice_logs . | ||
| clean_case_logs . |
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partitioned-pipe-multiscale/fluid1d-left-nutils/requirements.txt
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| setuptools # required by nutils | ||
| nutils==9 | ||
| numpy >1, <2 | ||
| pyprecice~=3.0 | ||
| matplotlib |
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| @@ -0,0 +1,13 @@ | ||
| #!/usr/bin/env bash | ||
| set -e -u | ||
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| . ../../tools/log.sh | ||
| exec > >(tee --append "$LOGFILE") 2>&1 | ||
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| python3 -m venv .venv | ||
| . .venv/bin/activate | ||
| pip install -r requirements.txt && pip freeze > pip-installed-packages.log | ||
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| NUTILS_RICHOUTPUT=no python3 ../solver-fluid1d-nutils/Fluid1D.py side=Left | ||
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| close_log |
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| probes.txt | ||
| final_fields.txt |
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| #!/usr/bin/env sh | ||
| set -e -u | ||
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| . ../../tools/cleaning-tools.sh | ||
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| rm -f ./results/Fluid1D_* | ||
| rm -f ./probes.txt | ||
| rm -f ./final_fields.txt | ||
| clean_precice_logs . | ||
| clean_case_logs . |
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partitioned-pipe-multiscale/fluid1d-right-nutils/requirements.txt
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| setuptools # required by nutils | ||
| nutils==9 | ||
| numpy >1, <2 | ||
| pyprecice~=3.0 | ||
| matplotlib |
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| Original file line number | Diff line number | Diff line change |
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| @@ -0,0 +1,13 @@ | ||
| #!/usr/bin/env bash | ||
| set -e -u | ||
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| . ../../tools/log.sh | ||
| exec > >(tee --append "$LOGFILE") 2>&1 | ||
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| python3 -m venv .venv | ||
| . .venv/bin/activate | ||
| pip install -r requirements.txt && pip freeze > pip-installed-packages.log | ||
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| NUTILS_RICHOUTPUT=no python3 ../solver-fluid1d-nutils/Fluid1D.py side=Right | ||
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| close_log |
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