From 62ace52513e8fb3917f48f70cbb31a07af72ec28 Mon Sep 17 00:00:00 2001 From: Emily Bourne Date: Wed, 20 Nov 2024 22:51:10 +0100 Subject: [PATCH] Add a script to allow users to create a private fork Add a script to allow users to create a private fork on GitHub which automatically looks for updates in the GitHub repo and updates a main and a devel branch. See merge request gysela-developpers/gyselalibxx!776 -------------------------------------------- --- bin/create_private_fork | 164 +++ simulations/geometryXVx/CMakeLists.txt | 2 + simulations/geometryXVx/README.md | 4 +- .../geometryXVx/neutrals/CMakeLists.txt | 32 + simulations/geometryXVx/neutrals/README.md | 9 + simulations/geometryXVx/neutrals/neutrals.cpp | 342 +++++++ .../geometryXVx/neutrals/neutrals.yml.hpp | 86 ++ .../neutrals/pdi_out_neutrals.yml.hpp | 251 +++++ simulations/geometryXVx/sheath/CMakeLists.txt | 28 + simulations/geometryXVx/sheath/README.md | 29 + ...ergy_conservation_error_electrons_t5.0.png | Bin 0 -> 72109 bytes ...energy_conservation_error_electrons_xt.png | Bin 0 -> 42130 bytes .../energy_conservation_error_ions_t5.0.png | Bin 0 -> 54612 bytes .../energy_conservation_error_ions_xt.png | Bin 0 -> 32174 bytes ...mass_conservation_error_electrons_t5.0.png | Bin 0 -> 60079 bytes .../mass_conservation_error_electrons_xt.png | Bin 0 -> 40632 bytes .../mass_conservation_error_ions_t5.0.png | Bin 0 -> 48552 bytes .../mass_conservation_error_ions_xt.png | Bin 0 -> 28686 bytes ...ntum_conservation_error_electrons_t5.0.png | Bin 0 -> 55481 bytes ...mentum_conservation_error_electrons_xt.png | Bin 0 -> 40051 bytes .../momentum_conservation_error_ions_t5.0.png | Bin 0 -> 57963 bytes .../momentum_conservation_error_ions_xt.png | Bin 0 -> 35986 bytes .../geometryXVx/sheath/doc/library.bib | 953 ++++++++++++++++++ .../sheath/doc/sheath_equations.pdf | Bin 0 -> 236544 bytes .../sheath/doc/sheath_equations.tex | 87 ++ .../geometryXVx/sheath/pdi_out.yml.hpp | 195 ++++ .../figures/charge_density_t990.0.png | Bin 0 -> 67916 bytes .../electrostatic_potential_t990.0.png | Bin 0 -> 57394 bytes .../fdistribu_xv_electrons_t990.0_linear.png | Bin 0 -> 51796 bytes .../fdistribu_xv_ions_t990.0_linear.png | Bin 0 -> 64298 bytes .../figures/heat_flux_electrons_t990.0.png | Bin 0 -> 56272 bytes ...um_conservation_error_electrons_t990.0.png | Bin 0 -> 71297 bytes ...mentum_conservation_error_electrons_xt.png | Bin 0 -> 50643 bytes .../figures/particle_flux_ions_t990.0.png | Bin 0 -> 51933 bytes .../sheath/ref_simulation/sheath_ref.yaml | 53 + simulations/geometryXVx/sheath/sheath.cpp | 276 +++++ .../geometryXVx/sheath/sheath.yaml.hpp | 73 ++ src/geometryXVx/CMakeLists.txt | 2 + src/geometryXVx/README.md | 2 + src/geometryXVx/geometry/geometry.hpp | 5 - src/geometryXVx/geometryMX/CMakeLists.txt | 6 + src/geometryXVx/geometryMX/README.md | 8 + .../fluidinitialization/CMakeLists.txt | 23 + .../geometryMX/fluidinitialization/README.md | 6 + .../constantfluidinitialization.cpp | 24 + .../constantfluidinitialization.hpp | 30 + .../ifluidinitialization.hpp | 21 + .../fluidtransportsolver/CMakeLists.txt | 32 + .../geometryMX/fluidtransportsolver/README.md | 7 + .../diffusiveneutralsolver.cpp | 231 +++++ .../diffusiveneutralsolver.hpp | 137 +++ .../ifluidtransportsolver.hpp | 30 + .../fluidtransportsolver/nullfluidsolver.cpp | 20 + .../fluidtransportsolver/nullfluidsolver.hpp | 38 + .../kineticfluidcoupling/CMakeLists.txt | 30 + .../geometryMX/kineticfluidcoupling/README.md | 6 + .../ikineticfluidcoupling.hpp | 37 + .../kinetic_fluid_coupling_source.cpp | 229 +++++ .../kinetic_fluid_coupling_source.hpp | 124 +++ .../geometryMX/reactionrates/CMakeLists.txt | 29 + .../geometryMX/reactionrates/README.md | 10 + .../reactionrates/charge_exchange.cpp | 59 ++ .../reactionrates/charge_exchange.hpp | 47 + .../geometryMX/reactionrates/constantrate.cpp | 14 + .../geometryMX/reactionrates/constantrate.hpp | 35 + .../geometryMX/reactionrates/ionization.cpp | 55 + .../geometryMX/reactionrates/ionization.hpp | 48 + .../reactionrates/ireactionrate.hpp | 27 + .../reactionrates/ratecomputation.hpp | 62 ++ .../reactionrates/recombination.cpp | 46 + .../reactionrates/recombination.hpp | 48 + .../time_integration_hybrid/CMakeLists.txt | 29 + .../time_integration_hybrid/README.md | 15 + .../itimesolver_hybrid.hpp | 33 + .../predcorr_hybrid.cpp | 99 ++ .../predcorr_hybrid.hpp | 73 ++ tests/geometryXVx/CMakeLists.txt | 6 + tests/geometryXVx/geometryMX/CMakeLists.txt | 43 + .../geometryMX/diffusiveneutrals.cpp | 215 ++++ tests/geometryXVx/geometryMX/fluidspecies.cpp | 212 ++++ .../geometryMX/kineticfluidcoupling.cpp | 305 ++++++ tests/geometryXVx/geometryMX/moments.cpp | 143 +++ .../geometryMX/predcorr_hybrid.cpp | 275 +++++ .../geometryMX/ratecoefficients.cpp | 178 ++++ tests/geometryXVx/sheath/CMakeLists.txt | 27 + .../geometryXVx/sheath/test_sheath_restart.sh | 71 ++ .../test_sheath_restart_user_defined_grid.sh | 75 ++ 87 files changed, 5904 insertions(+), 7 deletions(-) create mode 100755 bin/create_private_fork create mode 100644 simulations/geometryXVx/neutrals/CMakeLists.txt create mode 100644 simulations/geometryXVx/neutrals/README.md create mode 100644 simulations/geometryXVx/neutrals/neutrals.cpp create mode 100644 simulations/geometryXVx/neutrals/neutrals.yml.hpp create mode 100644 simulations/geometryXVx/neutrals/pdi_out_neutrals.yml.hpp create mode 100644 simulations/geometryXVx/sheath/CMakeLists.txt create mode 100644 simulations/geometryXVx/sheath/README.md create mode 100644 simulations/geometryXVx/sheath/conservations_plots/energy_conservation_error_electrons_t5.0.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/energy_conservation_error_electrons_xt.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/energy_conservation_error_ions_t5.0.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/energy_conservation_error_ions_xt.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/mass_conservation_error_electrons_t5.0.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/mass_conservation_error_electrons_xt.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/mass_conservation_error_ions_t5.0.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/mass_conservation_error_ions_xt.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/momentum_conservation_error_electrons_t5.0.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/momentum_conservation_error_electrons_xt.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/momentum_conservation_error_ions_t5.0.png create mode 100644 simulations/geometryXVx/sheath/conservations_plots/momentum_conservation_error_ions_xt.png create mode 100644 simulations/geometryXVx/sheath/doc/library.bib create mode 100644 simulations/geometryXVx/sheath/doc/sheath_equations.pdf create mode 100644 simulations/geometryXVx/sheath/doc/sheath_equations.tex create mode 100644 simulations/geometryXVx/sheath/pdi_out.yml.hpp create mode 100644 simulations/geometryXVx/sheath/ref_simulation/figures/charge_density_t990.0.png create mode 100644 simulations/geometryXVx/sheath/ref_simulation/figures/electrostatic_potential_t990.0.png create mode 100644 simulations/geometryXVx/sheath/ref_simulation/figures/fdistribu_xv_electrons_t990.0_linear.png create mode 100644 simulations/geometryXVx/sheath/ref_simulation/figures/fdistribu_xv_ions_t990.0_linear.png create mode 100644 simulations/geometryXVx/sheath/ref_simulation/figures/heat_flux_electrons_t990.0.png create mode 100644 simulations/geometryXVx/sheath/ref_simulation/figures/momentum_conservation_error_electrons_t990.0.png create mode 100644 simulations/geometryXVx/sheath/ref_simulation/figures/momentum_conservation_error_electrons_xt.png create mode 100644 simulations/geometryXVx/sheath/ref_simulation/figures/particle_flux_ions_t990.0.png create mode 100644 simulations/geometryXVx/sheath/ref_simulation/sheath_ref.yaml create mode 100644 simulations/geometryXVx/sheath/sheath.cpp create mode 100644 simulations/geometryXVx/sheath/sheath.yaml.hpp create mode 100644 src/geometryXVx/geometryMX/CMakeLists.txt create mode 100644 src/geometryXVx/geometryMX/README.md create mode 100644 src/geometryXVx/geometryMX/fluidinitialization/CMakeLists.txt create mode 100644 src/geometryXVx/geometryMX/fluidinitialization/README.md create mode 100644 src/geometryXVx/geometryMX/fluidinitialization/constantfluidinitialization.cpp create mode 100644 src/geometryXVx/geometryMX/fluidinitialization/constantfluidinitialization.hpp create mode 100644 src/geometryXVx/geometryMX/fluidinitialization/ifluidinitialization.hpp create mode 100644 src/geometryXVx/geometryMX/fluidtransportsolver/CMakeLists.txt create mode 100644 src/geometryXVx/geometryMX/fluidtransportsolver/README.md create mode 100644 src/geometryXVx/geometryMX/fluidtransportsolver/diffusiveneutralsolver.cpp create mode 100644 src/geometryXVx/geometryMX/fluidtransportsolver/diffusiveneutralsolver.hpp create mode 100644 src/geometryXVx/geometryMX/fluidtransportsolver/ifluidtransportsolver.hpp create mode 100644 src/geometryXVx/geometryMX/fluidtransportsolver/nullfluidsolver.cpp create mode 100644 src/geometryXVx/geometryMX/fluidtransportsolver/nullfluidsolver.hpp create mode 100644 src/geometryXVx/geometryMX/kineticfluidcoupling/CMakeLists.txt create mode 100644 src/geometryXVx/geometryMX/kineticfluidcoupling/README.md create mode 100644 src/geometryXVx/geometryMX/kineticfluidcoupling/ikineticfluidcoupling.hpp create mode 100644 src/geometryXVx/geometryMX/kineticfluidcoupling/kinetic_fluid_coupling_source.cpp create mode 100644 src/geometryXVx/geometryMX/kineticfluidcoupling/kinetic_fluid_coupling_source.hpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/CMakeLists.txt create mode 100644 src/geometryXVx/geometryMX/reactionrates/README.md create mode 100644 src/geometryXVx/geometryMX/reactionrates/charge_exchange.cpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/charge_exchange.hpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/constantrate.cpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/constantrate.hpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/ionization.cpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/ionization.hpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/ireactionrate.hpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/ratecomputation.hpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/recombination.cpp create mode 100644 src/geometryXVx/geometryMX/reactionrates/recombination.hpp create mode 100644 src/geometryXVx/time_integration_hybrid/CMakeLists.txt create mode 100644 src/geometryXVx/time_integration_hybrid/README.md create mode 100644 src/geometryXVx/time_integration_hybrid/itimesolver_hybrid.hpp create mode 100644 src/geometryXVx/time_integration_hybrid/predcorr_hybrid.cpp create mode 100644 src/geometryXVx/time_integration_hybrid/predcorr_hybrid.hpp create mode 100644 tests/geometryXVx/geometryMX/CMakeLists.txt create mode 100644 tests/geometryXVx/geometryMX/diffusiveneutrals.cpp create mode 100644 tests/geometryXVx/geometryMX/fluidspecies.cpp create mode 100644 tests/geometryXVx/geometryMX/kineticfluidcoupling.cpp create mode 100644 tests/geometryXVx/geometryMX/moments.cpp create mode 100644 tests/geometryXVx/geometryMX/predcorr_hybrid.cpp create mode 100644 tests/geometryXVx/geometryMX/ratecoefficients.cpp create mode 100644 tests/geometryXVx/sheath/CMakeLists.txt create mode 100644 tests/geometryXVx/sheath/test_sheath_restart.sh create mode 100644 tests/geometryXVx/sheath/test_sheath_restart_user_defined_grid.sh diff --git a/bin/create_private_fork b/bin/create_private_fork new file mode 100755 index 000000000..4a1883e4d --- /dev/null +++ b/bin/create_private_fork @@ -0,0 +1,164 @@ +#!/bin/bash +# SPDX-License-Identifier: MIT + +# Check for the gh command +if ! command -v gh 2>&1 >/dev/null +then + echo "This script uses GitHub's command line tool 'gh' but it does not seem to be installed." + echo "The installation instructions can be found at https://github.com/cli/cli?tab=readme-ov-file#installation" + exit 1 +fi + +# Check that the gh command has been initialised +if ! gh auth status -h github.com >/dev/null +then + echo "Please run:" + echo "gh auth login -h github.com" + echo "To authenticate on GitHub for the first time. This will allow you to use the GitHub CLI to create new repositories" + exit 1 +fi + +# Create the directory for the new repository +set -e +echo "Please provide the path to the folder where you want to create the new repository:" + +read directory + +directory=$(realpath ${directory}) + +if [ -d "${directory}" ]; then + echo "The specified folder already exists." +fi + +# Clone the repository into the new folder +git clone git@github.com:gyselax/gyselalibxx.git --single-branch --branch main ${directory} + +echo "Created ${directory}" + +cd ${directory} + +git remote rename origin gyselalibxx + +# Create the new private repository +echo "What would you like to call your private repository ? [Default: gyselalibxx]" + +read repo_name + +if [ -z "${repo_name}" ]; then + repo_name=gyselalibxx +fi +echo ${repo_name} + +git_user=$(python3 -c "import subprocess; import json; p=subprocess.run(['gh', 'api', 'user'], capture_output=True, universal_newlines=True); d = json.loads(p.stdout); print(d['login'])") + +gh repo create --private ${repo_name} -r origin -s . + +# Setup the branches and default settings on the new private repository +gh repo set-default ${git_user}/${repo_name} +git push -u origin main + +git checkout -b devel +git push -u origin devel + +gh repo edit --default-branch devel --delete-branch-on-merge --enable-squash-merge --allow-update-branch +gh label create "Ready to review" -c "#F2DD28" -d "Label to be automatically added to a PR when it is ready to be reviewed" +gh label create "Ready to merge" -c "#A9F543" -d "Label to be automatically added to a PR when it is approved and tests are passing" +gh api \ + --method PUT \ + -H "Accept: application/vnd.github+json" \ + -H "X-GitHub-Api-Version: 2022-11-28" \ + /repos/${git_user}/${repo_name}/actions/permissions/workflow \ + -f "default_workflow_permissions=write" -F "can_approve_pull_request_reviews=true" + +# Create the CI to update the main and devel branches +cat >.github/workflows/mirror_files.yml <> \$GITHUB_OUTPUT + git checkout devel + set +e + ./bin/update_branches + SUCCESS=\$? + echo + set -e + existing_issue=\$(gh issue list -S "Update repository" --json number) + if [[ \${SUCCESS} != 0 ]] + then + if [[ "\${existing_issue}" == "[]" ]] + then + gh issue create -t "Update repository" -b "This repository has conflicts with the main repository. Please run ./bin/update_branches and fix rebase conflicts manually" + fi + else + if [[ "\${existing_issue}" != "[]" ]] + then + issue_id=\$(python -c "import json; print(json.loads('\${existing_issue}'[1:-1])['number'])") + gh issue close \${issue_id} -r completed -c "Fixed as of \$(date)" + fi + fi + shell: bash + env: + GH_TOKEN: \${{ github.token }} +EOL + +cat >bin/update_branches < /dev/null; then + git remote add gyselalibxx git@github.com:gyselax/gyselalibxx.git +fi +git merge gyselalibxx/main +git checkout devel + +git rebase --onto main \${MAIN_SHA} devel +SUCCESS=\$? + +if [[ \${SUCCESS} == 0 ]] +then + git push -f --all + echo "Main and devel branch updated successfully" +else + git status + exit 1 +fi +EOL +chmod +x bin/update_branches +git add bin/update_branches .github/workflows/mirror_files.yml +git commit -m "Set up repository mirroring" +git push + +# Output explanations to user +RED='\033[0;31m' +NC='\033[0m' # No Color + +echo -e "The new repository was created successfully." +echo -e "This repository contains 2 branches:" +echo -e "- main" +echo -e "- devel" +echo -e "" +echo -e "The main branch is a duplicate of the main branch in the gyselax/gyselalibxx repository." +echo -e "${RED}The main branch should not be modified manually.${NC}" +echo -e "The devel branch contains clean commits which can be added to the main branch in the gyselax/gyselalibxx repository when the developments in this branch become public." +echo -e "In order to develop in this repository you should create a third branch for your developments. When you are happy with the changes you can create a pull request and merge them cleanly into the devel branch." +echo -e "At 3:00 every morning a CI will run on GitHub to update the main branch and rebase the devel branch onto the main branch. This will ensure that your developments remain up to date with the gyselax/gyselalibxx repository. If the rebase fails then an issue will be created to warn you to fix this problem manually." +echo -e "This repository is private and can only be accessed by other developers if you give them permission in the settings." +echo -e "If you need to make general changes to gyselalibxx which are not private and could be useful for other users please try to create issues directly in the gyselax/gyselalibxx repository. Once the pull request has been merged there you can update your branches (without waiting for 3:00 am by running ./bin/update_branches" diff --git a/simulations/geometryXVx/CMakeLists.txt b/simulations/geometryXVx/CMakeLists.txt index cad403c66..e6f6338cf 100644 --- a/simulations/geometryXVx/CMakeLists.txt +++ b/simulations/geometryXVx/CMakeLists.txt @@ -2,3 +2,5 @@ add_subdirectory(landau) add_subdirectory(bump_on_tail) +add_subdirectory(neutrals) +add_subdirectory(sheath) diff --git a/simulations/geometryXVx/README.md b/simulations/geometryXVx/README.md index b77e3cd60..4e8df19ab 100644 --- a/simulations/geometryXVx/README.md +++ b/simulations/geometryXVx/README.md @@ -2,5 +2,5 @@ This folder constains the following simulations: -- Landau -- Bump-On-Tail +- [sheath](./sheath/README.md) - A Boltzmann-Poisson system is solved for the electric field and the distribution function for both electrons and ions species. +- [neutrals](./neutrals/README.md) - Executables for the study of plasma-neutral interactions on a single magnetic field line. diff --git a/simulations/geometryXVx/neutrals/CMakeLists.txt b/simulations/geometryXVx/neutrals/CMakeLists.txt new file mode 100644 index 000000000..2b1556e25 --- /dev/null +++ b/simulations/geometryXVx/neutrals/CMakeLists.txt @@ -0,0 +1,32 @@ +# SPDX-License-Identifier: MIT + +foreach(GEOMETRY_VARIANT IN LISTS GEOMETRY_XVx_VARIANTS_LIST) + +add_executable(neutrals_${GEOMETRY_VARIANT} neutrals.cpp) +target_link_libraries(neutrals_${GEOMETRY_VARIANT} + PUBLIC + DDC::DDC + DDC::PDI_Wrapper + gslx::advection + gslx::boltzmann_${GEOMETRY_VARIANT} + gslx::fluidinitialization_${GEOMETRY_VARIANT} + gslx::fluidsolver_${GEOMETRY_VARIANT} + gslx::moments + gslx::initialization_${GEOMETRY_VARIANT} + gslx::interpolation + gslx::paraconfpp + gslx::poisson_${GEOMETRY_VARIANT} + gslx::reactionrates_${GEOMETRY_VARIANT} + gslx::rhs_${GEOMETRY_VARIANT} + gslx::speciesinfo + gslx::time_integration_hybrid_${GEOMETRY_VARIANT} + gslx::io + gslx::utils + + paraconf::paraconf + PDI::pdi +) + +install(TARGETS neutrals_${GEOMETRY_VARIANT}) + +endforeach() diff --git a/simulations/geometryXVx/neutrals/README.md b/simulations/geometryXVx/neutrals/README.md new file mode 100644 index 000000000..21cd61ab5 --- /dev/null +++ b/simulations/geometryXVx/neutrals/README.md @@ -0,0 +1,9 @@ +# Neutral simulations + +## Description +The `neutral` executable allows the study of plasma-neutral interactions on a single magnetic field line. The magnetic field line is connected at both of its ends to a solid wall. A Boltzmann-Poisson system is solved for the electric field and the distribution function for both electrons and ions species. The model is one dimensional in space and velocity (1D1V). + +The wall region is treated using immersed boundary condition (or penalization). Electrons and ions are absorbed inside this region. The inertia difference between the two species drives the appearance of a positively charged layer (the sheath) at the plasma boundary. The neutrals are treated using a simple fluid model (advective, pressure-diffusion, etc.) + +## Usage +After building the code, run the executable located in `build/simulations/neutral/`. To use the default simulation parameters the user can provide the `--dump-config` option when launching the executable. \ No newline at end of file diff --git a/simulations/geometryXVx/neutrals/neutrals.cpp b/simulations/geometryXVx/neutrals/neutrals.cpp new file mode 100644 index 000000000..0a40bf5e6 --- /dev/null +++ b/simulations/geometryXVx/neutrals/neutrals.cpp @@ -0,0 +1,342 @@ +// SPDX-License-Identifier: MIT +#include +#include +#include +#include +#include +#include +#include +#include +#include +#include + +#include +#include + +#include +#include + +#include "bsl_advection_vx.hpp" +#include "bsl_advection_x.hpp" +#include "charge_exchange.hpp" +#include "chargedensitycalculator.hpp" +#include "collisions_inter.hpp" +#include "collisions_intra.hpp" +#include "constantfluidinitialization.hpp" +#include "constantrate.hpp" +#include "ddc_alias_inline_functions.hpp" +#include "diffusiveneutralsolver.hpp" +#include "fem_1d_poisson_solver.hpp" +#include "fft_poisson_solver.hpp" +#include "geometry.hpp" +#include "input.hpp" +#include "ionization.hpp" +#include "irighthandside.hpp" +#include "kinetic_fluid_coupling_source.hpp" +#include "kinetic_source.hpp" +#include "krook_source_adaptive.hpp" +#include "krook_source_constant.hpp" +#include "maxwellianequilibrium.hpp" +#include "neumann_spline_quadrature.hpp" +#include "neutrals.yml.hpp" +#include "output.hpp" +#include "paraconfpp.hpp" +#include "pdi_out_neutrals.yml.hpp" +#include "predcorr_hybrid.hpp" +#include "qnsolver.hpp" +#include "recombination.hpp" +#include "restartinitialization.hpp" +#include "singlemodeperturbinitialization.hpp" +#include "species_info.hpp" +#include "species_init.hpp" +#include "spline_interpolator.hpp" +#include "splitrighthandsidesolver.hpp" +#include "splitvlasovsolver.hpp" + +using std::cerr; +using std::endl; +using std::chrono::steady_clock; +namespace fs = std::filesystem; + +int main(int argc, char** argv) +{ + // Environments variables for profiling + setenv("KOKKOS_TOOLS_LIBS", KP_KERNEL_TIMER_PATH, false); + setenv("KOKKOS_TOOLS_TIMER_JSON", "true", false); + + long int iter_start; + PC_tree_t conf_voicexx; + parse_executable_arguments( + conf_voicexx, + iter_start, + argc, + argv, + (std::string(mesh_params_yaml) + std::string(params_yaml)).c_str()); + PC_tree_t conf_pdi = PC_parse_string(PDI_CFG); + PC_errhandler(PC_NULL_HANDLER); + PDI_init(conf_pdi); + + Kokkos::ScopeGuard kokkos_scope(argc, argv); + ddc::ScopeGuard ddc_scope(argc, argv); + +#ifdef INPUT_MESH + std::string spline_mesh_filename(PCpp_string(conf_voicexx, ".SplineMesh.grid_file")); + size_t spline_mesh_filename_size = spline_mesh_filename.size(); + PDI_multi_expose( + "setFilename", + "filename_size", + &spline_mesh_filename_size, + PDI_OUT, + "filename", + spline_mesh_filename.c_str(), + PDI_OUT, + NULL); +#endif + + // Reading config + // --> Mesh info + IdxRangeX const mesh_x = init_spline_dependent_idx_range< + GridX, + BSplinesX, + SplineInterpPointsX>(conf_voicexx, "x"); + IdxRangeVx const mesh_vx = init_spline_dependent_idx_range< + GridVx, + BSplinesVx, + SplineInterpPointsVx>(conf_voicexx, "vx"); + IdxRangeXVx const meshXVx(mesh_x, mesh_vx); + + SplineXBuilder const builder_x(meshXVx); +#if !defined(PERIODIC_RDIMX) || defined(INPUT_MESH) + SplineXBuilder_1d const builder_x_poisson(mesh_x); +#endif + SplineVxBuilder const builder_vx(meshXVx); + + IdxRangeSp idx_range_kinsp; + IdxRangeSp idx_range_fluidsp; + init_species_withfluid(idx_range_kinsp, idx_range_fluidsp, conf_voicexx); + + // Initialization of kinetic species distribution function + IdxRangeSpVx const meshSpVx(idx_range_kinsp, mesh_vx); + DFieldMemSpVx allfequilibrium(meshSpVx); + MaxwellianEquilibrium const init_fequilibrium + = MaxwellianEquilibrium::init_from_input(idx_range_kinsp, conf_voicexx); + init_fequilibrium(allfequilibrium); + + ddc::expose_to_pdi("iter_start", iter_start); + + IdxRangeSpXVx const meshSpXVx(idx_range_kinsp, meshXVx); + DFieldMemSpXVx allfdistribu(meshSpXVx); + double time_start(0); + if (iter_start == 0) { + SingleModePerturbInitialization const init = SingleModePerturbInitialization:: + init_from_input(allfequilibrium, idx_range_kinsp, conf_voicexx); + init(allfdistribu); + } else { + RestartInitialization const restart(iter_start, time_start); + restart(allfdistribu); + } + auto allfequilibrium_host = ddc::create_mirror_view_and_copy(get_field(allfequilibrium)); + + // Moments index range initialization + IdxStepMom const nb_fluid_moments(1); + IdxRangeMom const meshM(IdxMom(0), nb_fluid_moments); + ddc::init_discrete_space(); + + // Neutral species initialization + DFieldMemSpMomX neutrals_alloc(IdxRangeSpMomX(idx_range_fluidsp, meshM, mesh_x)); + DFieldSpMomX neutrals = get_field(neutrals_alloc); + host_t moments_init_host(IdxRangeSpMom(idx_range_fluidsp, meshM)); + + for (IdxSp const isp : idx_range_fluidsp) { + PC_tree_t const conf_nisp = PCpp_get( + conf_voicexx, + ".NeutralSpeciesInfo[%d]", + (isp - idx_range_fluidsp.front()).value()); + ddc::parallel_fill(moments_init_host[isp], PCpp_double(conf_nisp, ".density_eq")); + } + ConstantFluidInitialization fluid_init(get_const_field(moments_init_host)); + fluid_init(neutrals); + + // --> Algorithm info + double const deltat = PCpp_double(conf_voicexx, ".Algorithm.deltat"); + int const nbiter = static_cast(PCpp_int(conf_voicexx, ".Algorithm.nbiter")); + + // --> Output info + double const time_diag = PCpp_double(conf_voicexx, ".Output.time_diag"); + int const nbstep_diag = int(time_diag / deltat); + +#ifdef PERIODIC_RDIMX + ddc::PeriodicExtrapolationRule bv_x_min; + ddc::PeriodicExtrapolationRule bv_x_max; +#else + ddc::ConstantExtrapolationRule bv_x_min(ddc::coordinate(mesh_x.front())); + ddc::ConstantExtrapolationRule bv_x_max(ddc::coordinate(mesh_x.back())); +#endif + + ddc::ConstantExtrapolationRule bv_vx_min(ddc::coordinate(mesh_vx.front())); + ddc::ConstantExtrapolationRule bv_vx_max(ddc::coordinate(mesh_vx.back())); + + // Creating operators + SplineXEvaluator const spline_x_evaluator(bv_x_min, bv_x_max); + SplineVxEvaluator const spline_vx_evaluator(bv_vx_min, bv_vx_max); +#if !defined(PERIODIC_RDIMX) || defined(INPUT_MESH) + SplineXEvaluator_1d const spline_x_evaluator_poisson(bv_x_min, bv_x_max); +#endif + PreallocatableSplineInterpolator const spline_x_interpolator(builder_x, spline_x_evaluator); + PreallocatableSplineInterpolator const spline_vx_interpolator(builder_vx, spline_vx_evaluator); + + BslAdvectionSpatial const advection_x(spline_x_interpolator); + BslAdvectionVelocity const advection_vx(spline_vx_interpolator); + + // list of rhs operators + std::vector> rhs_operators; + std::vector krook_source_constant_vector; + std::vector krook_source_adaptive_vector; + // Krook operators initialization + int const nb_rhsKrook(PCpp_len(conf_voicexx, ".Krook")); + for (int ik = 0; ik < nb_rhsKrook; ++ik) { + // --> Krook info + PC_tree_t const conf_krook = PCpp_get(conf_voicexx, ".Krook[%d]", ik); + + static std::map + str2rhstype {{"source", RhsType::Source}, {"sink", RhsType::Sink}}; + RhsType type = str2rhstype[PCpp_string(conf_krook, ".type")]; + std::string const krook_name = PCpp_string(conf_krook, ".name"); + if (krook_name == "constant") { + krook_source_constant_vector.emplace_back( + mesh_x, + mesh_vx, + type, + PCpp_double(conf_krook, ".extent"), + PCpp_double(conf_krook, ".stiffness"), + PCpp_double(conf_krook, ".amplitude"), + PCpp_double(conf_krook, ".density"), + PCpp_double(conf_krook, ".temperature")); + rhs_operators.emplace_back(krook_source_constant_vector.back()); + + } else if (krook_name == "adaptive") { + krook_source_adaptive_vector.emplace_back( + mesh_x, + mesh_vx, + type, + PCpp_double(conf_krook, ".extent"), + PCpp_double(conf_krook, ".stiffness"), + PCpp_double(conf_krook, ".amplitude"), + PCpp_double(conf_krook, ".density"), + PCpp_double(conf_krook, ".temperature")); + rhs_operators.emplace_back(krook_source_adaptive_vector.back()); + } else { + throw std::invalid_argument( + "Invalid krook name, allowed values are: 'constant', or 'adaptive'."); + } + } + + // Kinetic source + KineticSource const rhs_kinetic_source( + mesh_x, + mesh_vx, + PCpp_double(conf_voicexx, ".KineticSource.extent"), + PCpp_double(conf_voicexx, ".KineticSource.stiffness"), + PCpp_double(conf_voicexx, ".KineticSource.amplitude"), + PCpp_double(conf_voicexx, ".KineticSource.density"), + PCpp_double(conf_voicexx, ".KineticSource.energy"), + PCpp_double(conf_voicexx, ".KineticSource.temperature")); + rhs_operators.emplace_back(rhs_kinetic_source); + + + CollisionsIntra const + collisions_intra(meshSpXVx, PCpp_double(conf_voicexx, ".CollisionsInfo.nustar0")); + rhs_operators.emplace_back(collisions_intra); + + std::optional collisions_inter; + if (PCpp_bool(conf_voicexx, ".CollisionsInfo.enable_inter")) { + collisions_inter.emplace(meshSpXVx, PCpp_double(conf_voicexx, ".CollisionsInfo.nustar0")); + rhs_operators.emplace_back(*collisions_inter); + } + SplitVlasovSolver const vlasov(advection_x, advection_vx); + SplitRightHandSideSolver const boltzmann(vlasov, rhs_operators); + + DFieldMemVx const quadrature_coeffs_alloc(neumann_spline_quadrature_coefficients< + Kokkos::DefaultExecutionSpace>(mesh_vx, builder_vx)); + ChargeDensityCalculator rhs(get_const_field(quadrature_coeffs_alloc)); +#if defined(PERIODIC_RDIMX) && !defined(INPUT_MESH) + FFTPoissonSolver poisson_solver(mesh_x); +#else + FEM1DPoissonSolver poisson_solver(builder_x_poisson, spline_x_evaluator_poisson); +#endif + QNSolver const poisson(poisson_solver, rhs); + + double const normalization_coeff + = PCpp_double(conf_voicexx, ".DiffusiveNeutralSolver.normalization_coeff_neutrals"); + double const norm_coeff_rate + = PCpp_double(conf_voicexx, ".DiffusiveNeutralSolver.norm_coeff_rate_neutrals"); + + // The CX coefficient needs to be first constructed in order to write a correct initstate file. Check pdi_out_neutrals.yml.hpp for a closer look. + ChargeExchangeRate charge_exchange(norm_coeff_rate); + IonizationRate ionization(norm_coeff_rate); + RecombinationRate recombination(norm_coeff_rate); + + SplineXBuilder_1d const spline_x_builder_neutrals(mesh_x); + SplineXEvaluator_1d const spline_x_evaluator_neutrals(bv_x_min, bv_x_max); + + DFieldMemVx const quadrature_coeffs_neutrals( + trapezoid_quadrature_coefficients(mesh_vx)); + + DiffusiveNeutralSolver const neutralsolver( + charge_exchange, + ionization, + recombination, + normalization_coeff, + spline_x_builder_neutrals, + spline_x_evaluator_neutrals, + get_const_field(quadrature_coeffs_neutrals)); + + KineticFluidCouplingSource const kineticfluidcoupling( + PCpp_double(conf_voicexx, ".KineticFluidCouplingSource.density_coupling_coeff"), + PCpp_double(conf_voicexx, ".KineticFluidCouplingSource.momentum_coupling_coeff"), + PCpp_double(conf_voicexx, ".KineticFluidCouplingSource.energy_coupling_coeff"), + ionization, + recombination, + normalization_coeff, + get_const_field(quadrature_coeffs_alloc)); + + PredCorrHybrid const predcorr(boltzmann, neutralsolver, poisson, kineticfluidcoupling); + + // Starting the code + ddc::expose_to_pdi("Nx_spline_cells", ddc::discrete_space().ncells()); + ddc::expose_to_pdi("Nvx_spline_cells", ddc::discrete_space().ncells()); + expose_mesh_to_pdi("MeshX", mesh_x); + expose_mesh_to_pdi("MeshVx", mesh_vx); + ddc::expose_to_pdi("Lx", ddcHelper::total_interval_length(mesh_x)); + ddc::expose_to_pdi("nbstep_diag", nbstep_diag); + ddc::expose_to_pdi("Nkinspecies", idx_range_kinsp.size()); + ddc::expose_to_pdi( + "fdistribu_charges", + ddc::discrete_space().charges()[idx_range_kinsp]); + ddc::expose_to_pdi( + "fdistribu_masses", + ddc::discrete_space().masses()[idx_range_kinsp]); + ddc::expose_to_pdi( + "neutrals_masses", + ddc::discrete_space().masses()[idx_range_fluidsp]); + ddc::expose_to_pdi("normalization_coeff_neutrals", normalization_coeff); + ddc::expose_to_pdi("norm_coeff_rate_neutrals", norm_coeff_rate); + ddc::PdiEvent("initial_state").with("fdistribu_eq", allfequilibrium_host); + + steady_clock::time_point const start = steady_clock::now(); + + predcorr(allfdistribu, neutrals, time_start, deltat, nbiter); + + steady_clock::time_point const end = steady_clock::now(); + + double const simulation_time = std::chrono::duration(end - start).count(); + std::cout << "Simulation time: " << simulation_time << "s\n"; + + PC_tree_destroy(&conf_pdi); + + PDI_finalize(); + + PC_tree_destroy(&conf_voicexx); + + return EXIT_SUCCESS; +} diff --git a/simulations/geometryXVx/neutrals/neutrals.yml.hpp b/simulations/geometryXVx/neutrals/neutrals.yml.hpp new file mode 100644 index 000000000..5ac1e7cb6 --- /dev/null +++ b/simulations/geometryXVx/neutrals/neutrals.yml.hpp @@ -0,0 +1,86 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#ifdef INPUT_MESH +constexpr char const* const mesh_params_yaml = R"PARAMS_CFG(SplineMesh: + x_min: 0.0 + x_max: 50 + x_ncells: 512 + vx_min: -6.0 + vx_max: +6.0 + vx_ncells: 256 + grid_file: "grids.h5" + +)PARAMS_CFG"; +#else +constexpr char const* const mesh_params_yaml = R"PARAMS_CFG(SplineMesh: + x_min: 0.0 + x_max: 50 + x_ncells: 512 + vx_min: -6.0 + vx_max: +6.0 + vx_ncells: 256 + +)PARAMS_CFG"; +#endif + +constexpr char const* const params_yaml = R"PARAMS_CFG(SpeciesInfo: +- charge: -1. + mass: 1. + density_eq: 1. + temperature_eq: 1. + mean_velocity_eq: 0. + perturb_amplitude: 0. + perturb_mode: 1 + +- charge: 1. + mass: 400. + density_eq: 1. + temperature_eq: 1. + mean_velocity_eq: 0. + perturb_amplitude: 0. + perturb_mode: 1 + +NeutralSpeciesInfo: +- mass: 400. + density_eq: 1. + +Krook: +- name: 'adaptive' # 'constant' or adaptive': constant values or not for nu coeff. + type: 'sink' + solver: 'rk2' # possible values : 'rk2' + extent: 0.20 + stiffness: 1 + amplitude: 0.1 + density: 1e-9 + temperature: 0.5 + +KineticSource: + extent: 0.45 + stiffness: 4 + amplitude: 0.1 + density: 1. + energy: 1. + temperature: 1. + +DiffusiveNeutralSolver: + normalization_coeff_neutrals: 1e-2 + norm_coeff_rate_neutrals: 1e-3 + +KineticFluidCouplingSource: + density_coupling_coeff: 1.0 + momentum_coupling_coeff: 0.0 + energy_coupling_coeff: 0.0 + +CollisionsInfo: + enable_inter: true + nustar0: 0.1 + +Algorithm: + deltat: 0.1 + nbiter: 50 + +Output: + time_diag: 0.1 +)PARAMS_CFG"; diff --git a/simulations/geometryXVx/neutrals/pdi_out_neutrals.yml.hpp b/simulations/geometryXVx/neutrals/pdi_out_neutrals.yml.hpp new file mode 100644 index 000000000..165dc0149 --- /dev/null +++ b/simulations/geometryXVx/neutrals/pdi_out_neutrals.yml.hpp @@ -0,0 +1,251 @@ +// SPDX-License-Identifier: MIT +#pragma once + +constexpr char const* const PDI_CFG = R"PDI_CFG( +metadata: + Nx_spline_cells : int + Nvx_spline_cells : int + iter : int + iter_start : int + time_saved : double + nbstep_diag: int + iter_saved : int + Lx : double + grid_x_extents: { type: array, subtype: int64, size: 1 } + grid_x: + type: array + subtype: double + size: [ '$grid_x_extents[0]' ] + grid_vx_extents: { type: array, subtype: int64, size: 1 } + grid_vx: + type: array + subtype: double + size: [ '$grid_vx_extents[0]' ] + MeshX_extents: { type: array, subtype: int64, size: 1 } + MeshX: + type: array + subtype: double + size: [ '$MeshX_extents[0]' ] + MeshVx_extents: { type: array, subtype: int64, size: 1 } + MeshVx: + type: array + subtype: double + size: [ '$MeshVx_extents[0]' ] + Nkinspecies: int + fdistribu_charges_extents : { type: array, subtype: int64, size: 1 } + fdistribu_charges: + type: array + subtype: double + size: [ '$fdistribu_charges_extents[0]' ] + fdistribu_masses_extents : { type: array, subtype: int64, size: 1 } + fdistribu_masses: + type: array + subtype: double + size: [ '$fdistribu_masses_extents[0]' ] + neutrals_masses_extents: { type: array, subtype: int64, size: 1 } + neutrals_masses: + type: array + subtype: double + size: [ '$neutrals_masses_extents[0]' ] + fdistribu_eq_extents : { type: array, subtype: int64, size: 2 } + fdistribu_eq: + type: array + subtype: double + size: [ '$fdistribu_eq_extents[0]', '$fdistribu_eq_extents[1]' ] + collintra_nustar0 : double + collinter_nustar0 : double + normalization_coeff_neutrals : double + norm_coeff_rate_neutrals : double + charge_exchange_coefficients: + type: array + subtype: double + size: [ 5 ] + ionization_slope_coefficients: + type: array + subtype: double + size: [ 6 ] + ionization_intercept_coefficients: + type: array + subtype: double + size: [ 6 ] + recombination_slope_coefficients: + type: array + subtype: double + size: [ 2 ] + recombination_intercept_coefficients: + type: array + subtype: double + size: [ 2 ] + + krook_sink_adaptive_extent : double + krook_sink_adaptive_stiffness : double + krook_sink_adaptive_amplitude : double + krook_sink_adaptive_density : double + krook_sink_adaptive_temperature : double + krook_sink_adaptive_mask_extents: { type: array, subtype: int64, size: 1 } + krook_sink_adaptive_mask: + type: array + subtype: double + size: [ '$krook_sink_adaptive_mask_extents[0]' ] + krook_sink_adaptive_ftarget_extents: { type: array, subtype: int64, size: 1 } + krook_sink_adaptive_ftarget: + type: array + subtype: double + size: [ '$krook_sink_adaptive_ftarget_extents[0]' ] + + krook_sink_constant_extent : double + krook_sink_constant_stiffness : double + krook_sink_constant_amplitude : double + krook_sink_constant_density : double + krook_sink_constant_temperature : double + krook_sink_constant_mask_extents: { type: array, subtype: int64, size: 1 } + krook_sink_constant_mask: + type: array + subtype: double + size: [ '$krook_sink_constant_mask_extents[0]' ] + krook_sink_constant_ftarget_extents: { type: array, subtype: int64, size: 1 } + krook_sink_constant_ftarget: + type: array + subtype: double + size: [ '$krook_sink_constant_ftarget_extents[0]' ] + + kinetic_source_extent : double + kinetic_source_stiffness : double + kinetic_source_amplitude : double + kinetic_source_density : double + kinetic_source_energy : double + kinetic_source_temperature : double + kinetic_source_velocity_shape_extents: { type: array, subtype: int64, size: 1 } + kinetic_source_velocity_shape: + type: array + subtype: double + size: [ '$kinetic_source_velocity_shape_extents[0]' ] + kinetic_source_spatial_extent_extents: { type: array, subtype: int64, size: 1 } + kinetic_source_spatial_extent: + type: array + subtype: double + size: [ '$kinetic_source_spatial_extent_extents[0]' ] + + filename_size: size_t + filename: {type: array, subtype: char, size: "$filename_size"} + +data: + fdistribu_extents: { type: array, subtype: int64, size: 3 } + fdistribu: + type: array + subtype: double + size: [ '$fdistribu_extents[0]', '$fdistribu_extents[1]', '$fdistribu_extents[2]' ] + fluid_moments_extents : { type: array, subtype: int64, size: 3 } + fluid_moments: + type: array + subtype: double + size: [ '$fluid_moments_extents[0]', '$fluid_moments_extents[1]', '$fluid_moments_extents[2]' ] + electrostatic_potential_extents: { type: array, subtype: int64, size: 1 } + electrostatic_potential: + type: array + subtype: double + size: [ '$electrostatic_potential_extents[0]' ] + +plugins: + set_value: + on_init: + - share: + - iter_saved: 0 + on_data: + iter: + - set: + - iter_saved: '${iter_start} + ${iter}/${nbstep_diag}' + on_finalize: + - release: [iter_saved] + decl_hdf5: + - file: 'VOICEXX_initstate.h5' + on_event: [cx_rate_coeff_pol_expose] + collision_policy: replace_and_warn + write: + - charge_exchange_coefficients + - file: 'VOICEXX_initstate.h5' + on_event: [i_rate_coeff_pol_expose] + collision_policy: write_into + write: + - ionization_slope_coefficients + - ionization_intercept_coefficients + - file: 'VOICEXX_initstate.h5' + on_event: [r_rate_coeff_pol_expose] + collision_policy: write_into + write: + - recombination_slope_coefficients + - recombination_intercept_coefficients + + - file: 'VOICEXX_initstate.h5' + on_event: [initial_state] + collision_policy: write_into + write: + - Nx_spline_cells + - Nvx_spline_cells + - MeshX + - MeshVx + - Lx + - nbstep_diag + - collintra_nustar0 + - collinter_nustar0 + - normalization_coeff_neutrals + - norm_coeff_rate_neutrals + + - Nkinspecies + - fdistribu_charges + - fdistribu_masses + - neutrals_masses + - fdistribu_eq + + - krook_sink_adaptive_extent + - krook_sink_adaptive_stiffness + - krook_sink_adaptive_amplitude + - krook_sink_adaptive_density + - krook_sink_adaptive_temperature + - krook_sink_adaptive_mask + - krook_sink_adaptive_ftarget + + - krook_sink_constant_extent + - krook_sink_constant_stiffness + - krook_sink_constant_amplitude + - krook_sink_constant_density + - krook_sink_constant_temperature + - krook_sink_constant_mask + - krook_sink_constant_ftarget + + - kinetic_source_extent + - kinetic_source_stiffness + - kinetic_source_amplitude + - kinetic_source_density + - kinetic_source_energy + - kinetic_source_temperature + - kinetic_source_velocity_shape + - kinetic_source_spatial_extent + + + - file: 'VOICEXX_${iter_saved:05}.h5' + on_event: [iteration, last_iteration] + when: '${iter} % ${nbstep_diag} = 0' + collision_policy: replace_and_warn + write: [time_saved, fdistribu, fluid_moments, electrostatic_potential] + - file: 'VOICEXX_${iter_start:05}.h5' + on_event: restart + read: [time_saved, fdistribu] + - file: '${filename}' + on_event: [read_x_extents] + read: + grid_x_extents: {size_of: grid_x} + - file: '${filename}' + on_event: [read_x] + read: + grid_x: ~ + - file: '${filename}' + on_event: [read_vx_extents] + read: + grid_vx_extents: {size_of: grid_vx} + - file: '${filename}' + on_event: [read_vx] + read: + grid_vx: ~ + #trace: ~ +)PDI_CFG"; diff --git a/simulations/geometryXVx/sheath/CMakeLists.txt b/simulations/geometryXVx/sheath/CMakeLists.txt new file mode 100644 index 000000000..b4279e007 --- /dev/null +++ b/simulations/geometryXVx/sheath/CMakeLists.txt @@ -0,0 +1,28 @@ +# SPDX-License-Identifier: MIT + +foreach(GEOMETRY_VARIANT IN LISTS GEOMETRY_XVx_VARIANTS_LIST) + +add_executable(sheath_${GEOMETRY_VARIANT} sheath.cpp) +target_link_libraries(sheath_${GEOMETRY_VARIANT} + PUBLIC + DDC::DDC + DDC::PDI_Wrapper + gslx::initialization_${GEOMETRY_VARIANT} + gslx::interpolation + gslx::poisson_${GEOMETRY_VARIANT} + gslx::time_integration_${GEOMETRY_VARIANT} + gslx::speciesinfo + gslx::boltzmann_${GEOMETRY_VARIANT} + gslx::advection + gslx::paraconfpp + gslx::rhs_${GEOMETRY_VARIANT} + gslx::io + gslx::utils + + PDI::pdi + paraconf::paraconf + ) + +install(TARGETS sheath_${GEOMETRY_VARIANT}) + +endforeach() diff --git a/simulations/geometryXVx/sheath/README.md b/simulations/geometryXVx/sheath/README.md new file mode 100644 index 000000000..ee58ef064 --- /dev/null +++ b/simulations/geometryXVx/sheath/README.md @@ -0,0 +1,29 @@ +# Sheath simulations + +## Description +The `sheath` executable allows the study of kinetic plasma-wall interaction. A Boltzmann-Poisson system is solved for the electric field and the distribution function for both electrons and ions species. The model is one dimensional in space and velocity (1D1V). + +The particularity of the model lies in the description of the wall region, which is treated using immersed boundary condition (or penalization). Electrons and ions are absorbed inside this region. The inertia difference between the two species drives the appearance of a positively charged layer (the sheath) at the plasma boundary. More details about the sheath physics along with the need for non-equidistant meshes to conduct such simulations can be found in [1,2]. + +## Usage +After building the code, run the executable located in `build/simulations/sheath/`. To use the default simulation parameters the user can provide the `--dump-config` option when launching the executable. + +## Recommended parameters +Two sets of parameters are available : +- the default parameter given in `sheath.yaml.hpp`. This cas corresponds to a very light simulation case that runs a few iterations for testing purposes. This is the set of parameters that can be retrieved with the `--dump-config` command. +- the parameters given in the folder `ref_simulation`, in the `sheath_ref.yaml` file. This simulation presents a glimpse of the plasma-wall interaction physics that can be seen on the figures in the mentioned folder: formation of a positively charged layer in front of the wall region, accompanied by a drop of the electric potential that confines fast electrons. A particle flux going towards the wall exists in the plasma. With the number of iterations performed to obtain these figures, the system is not at steady state. To observe a steady state plasma-wall interaction with interesting physical features (supersonic flow of ions, truncation of fast velocity electrons, etc.) see the paramerers of [2]. + +## Verification of the simulation +The accuracy of the physical results from a sheath simulation can be verified as follows. The simulation should be run with the parameters given in `sheath.yaml.hpp` file. Then, any conservation diagnostic can be used to test the accuracy of the results. For instance, a post-process script that breaks down the terms present in the equation of energy conservation is `post-process/PythonScripts/geometryXVx/sheath/plot_conservation_energy`. This script can be run as an executable in the folder containing the simulation results. In the simple XVx geometry The equation of energy conservation is written as: + +$$\partial_t \Pi_a + 1/\sqrt{A_a}\, \partial_x Q_a - 2\Gamma_a q_a E/\sqrt{A_a} = S_{e}$$ + +Where $`\Gamma_a`$, $`\Pi_a`$ and $`Q_a`$ stand for the particle flux, momentum flux and energy flux of species $a$ (typically ions or electrons) respectively. These quantity are computed by the script using the distribution function of each species which is an output of the code. $`A_a = m_e/m_a`$ is the mass ratio of species $a$, and $`q_a`$ represents its charge ($+e$ for ions, $-e$ for electrons with $e$ the elementary charge). $E$ is the electric field, and $`S_{e}`$ the energy source term. The script plots all of the terms that appear in the energy conservation equation, along with the error (denoted as `lhs-rhs`) defined as being the left-hand-side term minus the right-hand-side terms, i.e. + +$$lhs-rhs = \partial_t \Pi_a + 1/\sqrt{A_a}\, \partial_x Q_a - 2\Gamma_a q_a E/\sqrt{A_a} - S_{e}.$$ + +This error term is plotted as well, and thus a simulation can be verified by ensuring that this error remains small as compared to the other terms. It is recommended to look at the conservation equation for electrons first, since as the lightest species, the numerical error is larger. The script also produces a 2D map of the error as a function of time and space. One shall note that in order to compute the time derivative term $`\partial_t \Pi_a`$, it is important to save all of the timesteps of the simulations, i.e. the parameters `time_diag` and `deltat` should be equal, as in the `sheath.yaml.hpp` file. Lastly, if one wishes to test a simulation that is faster, the number of iterations can be reduced to 10 for instance. The folder `conservation_plots` contains the graphs of the conservation equations computed using a simulation with the parameters of the `sheath.yaml.hpp` file. + +## References +- [1] E. Bourne, Y. Munschy, V. Grandgirard, M. Mehrenberger, and P. Ghendrih, Non-Uniform Splines for Semi-Lagrangian Kinetic Simulations of the Plasma Sheath (2022) +- [2] Y. Munschy, E. Bourne, P. Ghendrih, G. Dif-Pradalier, Y. Sarazin, V. Grandgirard, and P. 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z#l3C(53-Ptq*dT}&dRsW5j|q1zPa`RS?Kcg>C>+ZU4$F%6$GwSNG6XF$i8|b3M+$9 zpX(l!EhDiCh=psFlw!Q7bNotojoT(~f zX5xaMJNFs=b-zn^M(}Z8tXQL|9E>4JTYJKn#KRKo5A7nE<2Y<^y(YsGh5HYU#D%-h zVyU{fP(%~Yf<2U7y~kHi*3en{x15%py+lF#R`BENttZ<;$DIms1=>IT<1AU>B<}ZS z0VT)5{arcl^i|nT@2$F<-<%*jKS{_F%X?X=2WK)3{YYgYj-!)*i9UP#a{1zF5iG-k znCm)%hin5bLZieGcNACZO9nesPA}#q&?l0kA={v^8a7y^Nai$NGFiq+I8P*B2kEm9 zQ=#kB=w1>;pb2PtkQFAF8Ijf7hA78`)`xbX0*|H6XgIsbS&|zMcvMx-dJv%^_M5cr zd@qPmm?Vnx$H(6vni$yqQR859Y;rQ0Zjk2;$>3ea@{ca-9ETAS@E~|&GywJ3)C>C4oG0TMn-2dOJzhixOKaNtglPotnP^Kfe|0eTlmb#~dYxx?>?KNoc`t z4F;yB>zFpzUEW=@DY*2Wi^V)s5%eu12Ujh@H*t+7iZ+l1t^yQt`x8v) z$LZG}!}-aPBtQ8wdkifiiBHsG<7uLqQ^7XeYxO9j2qpJq^R}FiZ$D1Q_>HCP?n^Iv zRR`ZBXRZjwWx!@#wTQNb-IuJKCOl){iS>|qBwJ>o`;%R?*d`oCrwZbL(?`*Ym!FKR zq$b90J9Z(|1@A>K{{gzS2k0vIVF;@Y z(rPt8Shl$A+I_-w-0_L})OlH;gv;j{Z1XO~JnjLW7Y?B8XyZ*(=iM9=l|+9#0@ssD z*mbIII}BpamgsV9Wz1A(atwBN_c#{*xt#c(V6gev~A>3 z=3uy(CAb3JoGn{Z#%{82uK#+FVjaQH3.0.CO;2-K}, + abstract = {Abstract The boundary condition for ion fluid velocity at the magnetic presheath entrance is derived in the presence of the E ? B drift. This condition takes into account gradients of the drift velocity and di?er from the classical Bohm-Chodura condition.}, + number = {2-4}, + journal = {Contributions to Plasma Physics}, + author = {Tskhakaya, D and Kuhn, S}, + month = apr, + year = {2002}, + note = {Publisher: John Wiley \& Sons, Ltd}, + keywords = {\_tablet}, + pages = {302--308}, + file = {Tskhakaya_Kuhn_2002_Effect of E {\texttimes} B Drift on the Plasma Flow at the Magnetic Presheath Entrance.pdf:/home/ym266336/Zotero/storage/SZ3XSCJA/Tskhakaya_Kuhn_2002_Effect of E {\texttimes} B Drift on the Plasma Flow at the Magnetic Presheath Entrance.pdf:application/pdf}, +} + +@article{Brida2014, + title = {Investigation of {Oscillations} in the {Plasma} {Sheath}}, + volume = {54}, + doi = {10.1002/ctpp.201410038}, + journal = {Contributions to Plasma Physics}, + author = {Brida, D and Tskhakaya, David}, + month = jun, + year = {2014}, + keywords = {\_tablet}, + file = {Brida_Tskhakaya_2014_Investigation of Oscillations in the Plasma Sheath.pdf:/home/ym266336/Zotero/storage/NSW9FS77/Brida_Tskhakaya_2014_Investigation of Oscillations in the Plasma Sheath.pdf:application/pdf}, +} + +@article{Tskhakaya2014, + title = {Implementation of {PIC}/{MC} {Code} {BIT1} in {ITM} {Platform}}, + volume = {54}, + doi = {10.1002/ctpp.201410029}, + journal = {Contributions to Plasma Physics}, + author = {Tskhakaya, David and Coster, David and Contributors, Itm-tf}, + month = jun, + year = {2014}, + keywords = {\_tablet}, + file = {Tskhakaya et al_2014_Implementation of PIC-MC Code BIT1 in ITM Platform.pdf:/home/ym266336/Zotero/storage/KN8N4K4M/Tskhakaya et al_2014_Implementation of PIC-MC Code BIT1 in ITM Platform.pdf:application/pdf}, +} + +@book{Tskhakaya2010, + title = {{PIC}/{MC} code {BIT1} for plasma simulations on {HPC}}, + author = {Tskhakaya, David and Schneider, Ralf and Borchardt, Mariko and Soba, Alejandro and Yurtesen, Evren and Westerholm, Jan}, + month = mar, + year = {2010}, + doi = {10.1109/PDP.2010.47}, + note = {Publication Title: Proceedings of the 18th Euromicro Conference on Parallel, Distributed and Network-Based Processing, PDP 2010}, + keywords = {\_tablet}, + file = {Tskhakaya et al_2010_PIC-MC code BIT1 for plasma simulations on HPC.pdf:/home/ym266336/Zotero/storage/KN5XD7SA/Tskhakaya et al_2010_PIC-MC code BIT1 for plasma simulations on HPC.pdf:application/pdf}, +} + +@article{KOCAN2006, + title = {Particle simulations of the nonlinear electron dynamics in the classical {Pierce} diode}, + volume = {72}, + doi = {10.1017/S0022377806005010}, + journal = {Journal of Plasma Physics}, + author = {KOCAN, MARTIN and KUHN, S. and Tskhakaya, David and SKALN{\'Y}, J}, + month = dec, + year = {2006}, + keywords = {\_tablet}, + pages = {851--855}, + file = {KOCAN et al_2006_Particle simulations of the nonlinear electron dynamics in the classical Pierce.pdf:/home/ym266336/Zotero/storage/33TQ228H/KOCAN et al_2006_Particle simulations of the nonlinear electron dynamics in the classical Pierce.pdf:application/pdf}, +} + +@article{Tskhakaya2007, + title = {Optimization of {PIC} codes by improved memory management}, + volume = {225}, + issn = {0021-9991}, + url = {https://www.sciencedirect.com/science/article/pii/S002199910700006X}, + doi = {https://doi.org/10.1016/j.jcp.2007.01.002}, + abstract = {A simple method is described for optimization of particle-in-cell codes by improved memory management. This includes a faster calculation of Monte-Carlo collision operators. It is demonstrated that the CPU time can be reduced by a factor of 2 and more without reduction of the simulation accuracy.}, + number = {1}, + journal = {Journal of Computational Physics}, + author = {Tskhakaya, D and Schneider, R}, + year = {2007}, + keywords = {Binary collision, Monte Carlo, PIC, \_tablet}, + pages = {829--839}, + file = {Tskhakaya_Schneider_2007_Optimization of PIC codes by improved memory management.pdf:/home/ym266336/Zotero/storage/MSUK5XIJ/Tskhakaya_Schneider_2007_Optimization of PIC codes by improved memory management.pdf:application/pdf}, +} + +@article{Tskhakaya2007a, + title = {The {Particle}-{In}-{Cell} {Method}}, + volume = {47}, + issn = {0863-1042}, + url = {https://doi.org/10.1002/ctpp.200710072}, + doi = {https://doi.org/10.1002/ctpp.200710072}, + abstract = {Abstract This paper is the first in a series of three papers to summarize the recent work of an European-wide collaborationwhich is ongoing since about one decade using Particle-in-Cell (PIC) methods in low temperature plasma physics. In the present first paper the main aspects of this computational technique will be presented. In the second paper, an overview of applications in low-temperature plasma modelling will be given, whereas the third part will put emphasis on the specific results of modelling ion thrusters. (? 2008 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim)}, + number = {8-9}, + journal = {Contributions to Plasma Physics}, + author = {Tskhakaya, D and Matyash, K and Schneider, R and Taccogna, F}, + year = {2007}, + keywords = {PIC simulations, MC simulations, \_tablet}, + pages = {563--594}, + file = {Tskhakaya et al_2007_The Particle-In-Cell Method.pdf:/home/ym266336/Zotero/storage/WVVRDQAS/Tskhakaya et al_2007_The Particle-In-Cell Method.pdf:application/pdf}, +} + +@article{Tskhakaya2012, + title = {On {Recent} {Massively} {Parallelized} {PIC} {Simulations} of the {SOL}}, + volume = {52}, + issn = {0863-1042}, + url = {https://doi.org/10.1002/ctpp.201210038}, + doi = {https://doi.org/10.1002/ctpp.201210038}, + abstract = {Abstract Recent results of massively parallel kinetic (PIC/MC) simulations of the tokamak scrape-off layer are discussed. It is demonstrated that a number of well studied properties of the low-recycling divertor plasma, such as the sound speed and the average energy of plasma particles impinging on the divertors, cannot be generalized to the high recycling case. A new analytical model for plasma boundary condition has been derived (? 2012 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim)}, + number = {5-6}, + journal = {Contributions to Plasma Physics}, + author = {Tskhakaya, D}, + month = jun, + year = {2012}, + note = {Publisher: John Wiley \& Sons, Ltd}, + keywords = {PIC simulations, massively parallel modeling, SOL, \_tablet}, + pages = {490--499}, + file = {Tskhakaya_2012_On Recent Massively Parallelized PIC Simulations of the SOL.pdf:/home/ym266336/Zotero/storage/9ZBMFJHJ/Tskhakaya_2012_On Recent Massively Parallelized PIC Simulations of the SOL.pdf:application/pdf}, +} + +@article{ghendrih:hal-00848545, + title = {Transition to supersonic flows in the edge plasma}, + volume = {53}, + url = {https://hal.archives-ouvertes.fr/hal-00848545}, + doi = {10.1088/0741-3335/53/5/054019}, + number = {5}, + journal = {Plasma Physics and Controlled Fusion}, + author = {Ghendrih, Philippe and Bodi, K and Bufferand, Hugo and Chiavassa, Guillaume and Ciraolo, Guido and Fedorczak, Nicolas and Isoardi, Livia and Paredes, A and Sarazin, Yanick and Serre, Eric and Schwander, Fr{\'e}d{\'e}ric and Tamain, Patrick}, + year = {2011}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {54019}, + file = {Ghendrih et al_2011_Transition to supersonic flows in the edge plasma.pdf:/home/ym266336/Zotero/storage/M42X5Y4U/Ghendrih et al_2011_Transition to supersonic flows in the edge plasma.pdf:application/pdf}, +} + +@article{Riemann2012, + title = {Comment on {\textquoteleft}{Kinetic} theory of the presheath and the {Bohm} criterion{\textquoteright}}, + volume = {21}, + issn = {0963-0252}, + url = {http://dx.doi.org/10.1088/0963-0252/21/6/068001}, + doi = {10.1088/0963-0252/21/6/068001}, + abstract = {Recently, Baalrud and Hegna published a paper (2011 Plasma Sources Sci. Technol. 025013) claiming that the well-known kinetic Bohm criterion (BC) is based on two errors and suggested a new BC using exclusively positive-exponent velocity moments. It is shown that the paper conflicts with accepted sheath theory and that the v-2 velocity moment cannot be avoided in a rigorous asymptotic theory.}, + number = {6}, + journal = {Plasma Sources Science and Technology}, + author = {Riemann, K-U}, + year = {2012}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {68001}, + file = {Riemann_2012_Comment on {\textquoteleft}Kinetic theory of the presheath and the Bohm criterion{\textquoteright}.pdf:/home/ym266336/Zotero/storage/FK4QIEJ7/Riemann_2012_Comment on {\textquoteleft}Kinetic theory of the presheath and the Bohm criterion{\textquoteright}.pdf:application/pdf}, +} + +@article{Ulbl2021, + title = {Implementation and verification of a conservative, multi-species, gyro-averaged, full-f, {Lenard}-{Bernstein}/{Dougherty} collision operator in the gyrokinetic code {GENE}-{X}}, + volume = {n/a}, + issn = {0863-1042}, + url = {https://doi.org/10.1002/ctpp.202100180}, + doi = {https://doi.org/10.1002/ctpp.202100180}, + abstract = {Abstract Gyrokinetic simulations are among the main tools to predict turbulent transport in the core of fusion devices. Unlike the core, the plasma edge and scrape-off layer are characterized by lower temperature and higher collisionality. To allow for realistic gyrokinetic modelling of edge and scrape-off layer turbulence, it is crucial to include collisional effects into the simulations. In this work, we present a full-f, gyro-averaged, multi-species, Lenard-Bernstein/Dougherty (LBD) collision operator, for the use in the gyrokinetic turbulence code GENE-X. The operator accounts for exact particle density, momentum, and energy conservation, with collision frequencies chosen such that the momentum or temperature relaxation rates of the Boltzmann collision operator are recovered. We provide a conservative second-order finite-volume implementation of the operator and present a thorough verification. Due to the excellent conservation properties of the finite-volume implementation, it is possible to use a coarser velocity space grid, save computational resources and, as a consequence, perform simulations of larger fusion devices.}, + number = {n/a}, + journal = {Contributions to Plasma Physics}, + author = {Ulbl, Philipp and Michels, Dominik and Jenko, Frank}, + month = dec, + year = {2021}, + note = {Publisher: John Wiley \& Sons, Ltd}, + keywords = {collisions, GENE-X, gyrokinetics, \_tablet}, + pages = {e202100180}, + file = {Ulbl et al_2021_Implementation and verification of a conservative, multi-species,.pdf:/home/ym266336/Zotero/storage/B5J2BVBD/Ulbl et al_2021_Implementation and verification of a conservative, multi-species,.pdf:application/pdf}, +} + +@article{Shi2017, + title = {Gyrokinetic continuum simulation of turbulence in a straight open-field-line plasma}, + volume = {83}, + issn = {0022-3778}, + url = {https://www.cambridge.org/core/article/gyrokinetic-continuum-simulation-of-turbulence-in-a-straight-openfieldline-plasma/7E4273E83115F9ED55EDA393190D756F}, + doi = {DOI: 10.1017/S002237781700037X}, + abstract = {Five-dimensional gyrokinetic continuum simulations of electrostatic plasma turbulence in a straight, open-field-line geometry have been performed using a full- \$f\$ discontinuous-Galerkin approach implemented in the Gkeyll code. While various simplifications have been used for now, such as long-wavelength approximations in the gyrokinetic Poisson equation and the Hamiltonian, these simulations include the basic elements of a fusion-device scrape-off layer: localised sources to model plasma outflow from the core, cross-field turbulent transport, parallel flow along magnetic field lines, and parallel losses at the limiter or divertor with sheath-model boundary conditions. The set of sheath-model boundary conditions used in the model allows currents to flow through the walls. In addition to details of the numerical approach, results from numerical simulations of turbulence in the Large Plasma Device, a linear device featuring straight magnetic field lines, are presented.}, + number = {3}, + journal = {Journal of Plasma Physics}, + author = {Shi, E L and Hammett, G W and Stoltzfus-Dueck, T and Hakim, A}, + year = {2017}, + note = {Publisher: Cambridge University Press}, + keywords = {plasma heat loss, plasma sheaths, plasma simulation, \_tablet}, + pages = {905830304}, + file = {Shi et al_2017_Gyrokinetic continuum simulation of turbulence in a straight open-field-line.pdf:/home/ym266336/Zotero/storage/UXEDR7FN/Shi et al_2017_Gyrokinetic continuum simulation of turbulence in a straight open-field-line.pdf:application/pdf}, +} + +@article{Sarazin2011, + title = {Predictions on heat transport and plasma rotation from global gyrokinetic simulations}, + volume = {51}, + issn = {0029-5515}, + url = {http://dx.doi.org/10.1088/0029-5515/51/10/103023}, + doi = {10.1088/0029-5515/51/10/103023}, + abstract = {Flux-driven global gyrokinetic codes are now mature enough to make predictions in terms of turbulence and transport in tokamak plasmas. Some of the recent breakthroughs of three such codes, namely GYSELA, ORB5 and XGC1, are reported and compared wherever appropriate. In all three codes, turbulent transport appears to be mediated by avalanche-like events, for a broad range of $\rho$* = $\rho$i/a values, ratio of the gyro-radius over the minor radius. Still, the radial correlation length scales with $\rho$i, leading to the gyro-Bohm scaling of the effective transport coefficient below $\rho$* ? 1/300. The possible explanation could be due to the fact that avalanches remain meso-scale due to the interaction with zonal flows, whose characteristic radial wavelength appears to be almost independent of the system size. As a result of the radial corrugation of the turbulence driven zonal and mean flows, the shear of the radial electric field can be significantly underestimated if poloidal rotation is assumed to be governed by the neoclassical theory, especially at low collisionality. Indeed, the turbulence contribution to the poloidal rotation increases when collisionality decreases. Finally, the numerical verification of toroidal momentum balance shows that both neoclassical and turbulent contributions to the Reynolds' stress tensor play the dominant role. The phase space analysis further reveals that barely passing supra-thermal particles mostly contribute to the toroidal flow generation, consistently with quasi-linear predictions.}, + number = {10}, + journal = {Nuclear Fusion}, + author = {Sarazin, Y and Grandgirard, V and Abiteboul, J and Allfrey, S and Garbet, X and Ghendrih, Ph. and Latu, G and Strugarek, A and Dif-Pradalier, G and Diamond, P H and Ku, S and Chang, C S and McMillan, B F and Tran, T M and Villard, L and Jolliet, S and Bottino, A and Angelino, P}, + year = {2011}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {103023}, + file = {Sarazin et al_2011_Predictions on heat transport and plasma rotation from global gyrokinetic.pdf:/home/ym266336/Zotero/storage/LV735I9I/Sarazin et al_2011_Predictions on heat transport and plasma rotation from global gyrokinetic.pdf:application/pdf}, +} + +@article{Riemann1991, + title = {The {Bohm} criterion and sheath formation}, + volume = {24}, + issn = {0022-3727}, + url = {http://dx.doi.org/10.1088/0022-3727/24/4/001}, + doi = {10.1088/0022-3727/24/4/001}, + abstract = {In the limit of a small Debye length ( lambda D to 0) the analysis of the plasma boundary layer leads to a two-scale problem of a collision free sheath and of a quasi-neutral presheath. Bohm's criterion expresses a necessary condition for the formation of a stationary sheath in front of a negative absorbing wall. The basic features of the plasma-sheath transition and their relation to the Bohm criterion are discussed and illustrated from a simple cold-ion fluid model. A rigorous kinetic analysis of the vicinity of the sheath edge allows one to generalize Bohm's criterion accounting not only for arbitrary ion and electron distributions, but also for general boundary conditions at the wall. It is shown that the generalized sheath condition is (apart from special exceptions) marginally fulfilled and related to a sheath edge field singularity. Due to this singularity, smooth matching of the presheath and sheath solutions requires an additional transition layer. Previous investigations concerning particular problems of the plasma-sheath transition are reviewed in the light of the general relations.}, + number = {4}, + journal = {Journal of Physics D: Applied Physics}, + author = {Riemann, K -U}, + year = {1991}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {493--518}, + file = {Riemann_1991_The Bohm criterion and sheath formation.pdf:/home/ym266336/Zotero/storage/IUEK373T/Riemann_1991_The Bohm criterion and sheath formation.pdf:application/pdf}, +} + +@article{Riemann1996, + title = {Bohm's {Criterion} and {Plasma}-{Sheath} {Transition}}, + volume = {36}, + issn = {0863-1042}, + url = {https://doi.org/10.1002/ctpp.19960360105}, + doi = {https://doi.org/10.1002/ctpp.19960360105}, + abstract = {Abstract The general form of Bohm's condition for sheath formation (?D ? 0) and its relation to the plasma sheath transition is discussed both in the frames of a hydrodynamic and of a kinetic ion analysis. The sheath condition is usually fulfilled in the marginal (equality) form. Previous results for special problems are summarized.}, + number = {S1}, + journal = {Contributions to Plasma Physics}, + author = {Riemann, K.-U.}, + month = jan, + year = {1996}, + note = {Publisher: John Wiley \& Sons, Ltd}, + keywords = {\_tablet}, + pages = {19--27}, + file = {Riemann_1996_Bohm's Criterion and Plasma-Sheath Transition.pdf:/home/ym266336/Zotero/storage/799FQ6WJ/Riemann_1996_Bohm's Criterion and Plasma-Sheath Transition.pdf:application/pdf}, +} + +@article{Bhatnagar1954, + title = {A {Model} for {Collision} {Processes} in {Gases}. {I}. {Small} {Amplitude} {Processes} in {Charged} and {Neutral} {One}-{Component} {Systems}}, + volume = {94}, + url = {https://link.aps.org/doi/10.1103/PhysRev.94.511}, + doi = {10.1103/PhysRev.94.511}, + number = {3}, + journal = {Physical Review}, + author = {Bhatnagar, P L and Gross, E P and Krook, M}, + month = may, + year = {1954}, + note = {Publisher: American Physical Society}, + keywords = {\_tablet}, + pages = {511--525}, + file = {Bhatnagar et al_1954_A Model for Collision Processes in Gases.pdf:/home/ym266336/Zotero/storage/68BVAG7I/Bhatnagar et al_1954_A Model for Collision Processes in Gases.pdf:application/pdf}, +} + +@article{Wagner1982, + title = {Regime of {Improved} {Confinement} and {High} {Beta} in {Neutral}-{Beam}-{Heated} {Divertor} {Discharges} of the {ASDEX} {Tokamak}}, + volume = {49}, + url = {https://link.aps.org/doi/10.1103/PhysRevLett.49.1408}, + doi = {10.1103/PhysRevLett.49.1408}, + number = {19}, + journal = {Physical Review Letters}, + author = {Wagner, F and Becker, G and Behringer, K and Campbell, D and Eberhagen, A and Engelhardt, W and Fussmann, G and Gehre, O and Gernhardt, J and Gierke, G v. and Haas, G and Huang, M and Karger, F and Keilhacker, M and Kl{\"u}ber, O and Kornherr, M and Lackner, K and Lisitano, G and Lister, G G and Mayer, H M and Meisel, D and M{\"u}ller, E R and Murmann, H and Niedermeyer, H and Poschenrieder, W and Rapp, H and R{\"o}hr, H and Schneider, F and Siller, G and Speth, E and St{\"a}bler, A and Steuer, K H and Venus, G and Vollmer, O and Y{\"u}, Z}, + month = nov, + year = {1982}, + note = {Publisher: American Physical Society}, + keywords = {\_tablet}, + pages = {1408--1412}, + file = {Wagner et al_1982_Regime of Improved Confinement and High Beta in Neutral-Beam-Heated Divertor.pdf:/home/ym266336/Zotero/storage/CXJG8N83/Wagner et al_1982_Regime of Improved Confinement and High Beta in Neutral-Beam-Heated Divertor.pdf:application/pdf}, +} + +@inproceedings{difpradalier:cea-03287143, + address = {E-Conference, France}, + title = {Interplay between core, edge and scrape-off layer in turbulent magnetised plasmas}, + url = {https://hal-cea.archives-ouvertes.fr/cea-03287143}, + booktitle = {{FEC} 2020 - {IAEA} {Fusion} {Energy} {Conference}}, + author = {Dif-Pradalier, G and Ghendrih, Ph. and Sarazin, Y and Garbet, X and Grandgirard, V and Munschy, Y and Varennes, R and Vermare, L and Camenen, Y and Widmer, F}, + year = {2021}, + keywords = {\_tablet}, + file = {Dif-Pradalier et al_2021_Interplay between core, edge and scrape-off layer in turbulent magnetised.pdf:/home/ym266336/Zotero/storage/B4DBDSSX/Dif-Pradalier et al_2021_Interplay between core, edge and scrape-off layer in turbulent magnetised.pdf:application/pdf}, +} + +@article{Martin2008, + title = {Power requirement for accessing the {H}-mode in {ITER}}, + volume = {123}, + issn = {1742-6596}, + url = {http://dx.doi.org/10.1088/1742-6596/123/1/012033}, + doi = {10.1088/1742-6596/123/1/012033}, + abstract = {The input power requirements for accessing H-mode at low density and maintaining it during the density ramp in ITER is addressed by statistical means applied to the international H-mode threshold power database. Following the recent addition of new data, the improvement of existing data and the improvement of selection criteria, a revised scaling law that describes the threshold power required to obtain an L-mode to H-mode transition is presented. Predictions for ITER give a threshold power of \~{}52MW in a deuterium plasma at a line average density, ne = 0.5{\texttimes}1020m-3. At the nominal ITER H-mode density, ne = 1.0{\texttimes}1020m-3, the threshold power required is \~{}86MW. Detailed analysis of data from individual devices suggests that the density dependence of the threshold power might increase with the plasma size and the magnetic field. On the other hand, the density at which the threshold power is minimal is found to decrease with the plasma size and increase with magnetic field. The influence of these effects on the accessibility of the H-mode regime in ITER plasmas is discussed. Analyses of the confinement database show that, in present day devices, H-modes are generally maintained with powers exceeding the threshold power by a factor larger than 1.5, and that, on the other hand, good confinement can be obtained close to the threshold power although rarely demonstrated.}, + journal = {Journal of Physics: Conference Series}, + author = {Martin, Y R and Takizuka, T and Group, the ITPA CDBM H-mode Threshold Data}, + year = {2008}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {12033}, + file = {Martin et al_2008_Power requirement for accessing the H-mode in ITER.pdf:/home/ym266336/Zotero/storage/Z2GA9XJ2/Martin et al_2008_Power requirement for accessing the H-mode in ITER.pdf:application/pdf}, +} + +@article{Parker1993, + title = {A {Suitable} {Boundary} {Condition} for {Bounded} {Plasma} {Simulation} without {Sheath} {Resolution}}, + volume = {104}, + issn = {0021-9991}, + url = {https://www.sciencedirect.com/science/article/pii/S0021999183710053}, + doi = {https://doi.org/10.1006/jcph.1993.1005}, + abstract = {We have developed a technique that allows for a sheath boundary layer without having to resolve the inherently small space and time scales of the sheath region. We refer to this technique as the logical sheath boundary condition. This boundary condition, when incorporated into a direct-implicit particle code, permits large space- and time-scale simulations of bounded systems, which would otherwise be impractical on current supercomputers. The lack of resolution of the collector sheath potential drop obtained from conventional implicit simulations at moderate values of $\omega$pe $\Delta$t and $\Delta$ z/ $\lambda$De provides the motivation for the development of the logical sheath boundary condition. The algorithm for use of the logical sheath boundary condition in a particle simulation is presented. Results from simulations which use the logical sheath boundary condition are shown to compare reasonably well with those from an analytic theory and simulations in which the sheath is resolved.}, + number = {1}, + journal = {Journal of Computational Physics}, + author = {Parker, S E and Procassini, R J and Birdsall, C K and Cohen, B I}, + year = {1993}, + keywords = {\_tablet}, + pages = {41--49}, + file = {Parker et al_1993_A Suitable Boundary Condition for Bounded Plasma Simulation without Sheath.pdf:/home/ym266336/Zotero/storage/L9D8IZ4L/Parker et al_1993_A Suitable Boundary Condition for Bounded Plasma Simulation without Sheath.pdf:application/pdf}, +} + +@article{paredes:hal-01087225, + title = {A penalization technique to model plasma facing components in a tokamak with temperature variations}, + volume = {274}, + url = {https://hal.archives-ouvertes.fr/hal-01087225}, + journal = {Journal of Computational Physics}, + author = {Paredes, Alejandro and Bufferand, Hugo and Ciraolo, Guido and Schwander, Fr{\'e}d{\'e}ric and Serre, Eric and Ghendrih, Philippe and Tamain, Patrick}, + year = {2014}, + note = {Publisher: Elsevier}, + keywords = {Immersed boundary method, Penalization, Plasma--wall interaction, Scrape-off layer, Tokamak, \_tablet}, + pages = {283--298}, + file = {Paredes et al_2014_A penalization technique to model plasma facing components in a tokamak with.pdf:/home/ym266336/Zotero/storage/QGMB8AR4/Paredes et al_2014_A penalization technique to model plasma facing components in a tokamak with.pdf:application/pdf}, +} + +@techreport{donnel:hal-01687586, + title = {A multi-species collisional operator for full-{F} global gyrokinetics codes : {Numerical} aspects and validation with the {GYSELA} code}, + url = {https://hal.archives-ouvertes.fr/hal-01687586}, + author = {Donnel, Peter and Garbet, Xavier and Sarazin, Yanick and Grandgirard, Virginie and ASAHI, Yuuichi and Bouzat, Nicolas and CASCHERA, Elisabetta and Dif-Pradalier, Guilhem and Ehrlacher, Charles and Ghendrih, Philippe and Latu, Guillaume and Passeron, Chantal}, + year = {2018}, + keywords = {collision, H-theorem, multispecies, neoclassic, \_tablet}, + file = {Donnel et al_2018_A multi-species collisional operator for full-F global gyrokinetics codes.pdf:/home/ym266336/Zotero/storage/CMN5MKT9/Donnel et al_2018_A multi-species collisional operator for full-F global gyrokinetics codes.pdf:application/pdf}, +} + +@article{coulette:hal-01402204, + title = {Kinetic simulations of the {Chodura} and {Debye} sheaths for magnetic fields with grazing incidence}, + volume = {58}, + url = {https://hal.archives-ouvertes.fr/hal-01402204}, + doi = {10.1088/0741-3335/58/2/025008}, + number = {2}, + journal = {Plasma Physics and Controlled Fusion}, + author = {Coulette, David and Manfredi, Giovanni}, + year = {2016}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {25008}, + file = {Coulette_Manfredi_2016_Kinetic simulations of the Chodura and Debye sheaths for magnetic fields with.pdf:/home/ym266336/Zotero/storage/SRZ5L3EW/Coulette_Manfredi_2016_Kinetic simulations of the Chodura and Debye sheaths for magnetic fields with.pdf:application/pdf}, +} + +@article{Biglari1990, + title = {Influence of sheared poloidal rotation on edge turbulence}, + volume = {2}, + issn = {0899-8221}, + url = {https://doi.org/10.1063/1.859529}, + doi = {10.1063/1.859529}, + number = {1}, + journal = {Physics of Fluids B: Plasma Physics}, + author = {Biglari, H and Diamond, P H and Terry, P W}, + month = jan, + year = {1990}, + note = {Publisher: American Institute of Physics}, + keywords = {\_tablet}, + pages = {1--4}, + file = {Biglari et al_1990_Influence of sheared poloidal rotation on edge turbulence.pdf:/home/ym266336/Zotero/storage/PTA47HRF/Biglari et al_1990_Influence of sheared poloidal rotation on edge turbulence.pdf:application/pdf}, +} + +@article{Chodura1982, + title = {Plasma{\textendash}wall transition in an oblique magnetic field}, + volume = {25}, + issn = {0031-9171}, + url = {https://aip.scitation.org/doi/abs/10.1063/1.863955}, + doi = {10.1063/1.863955}, + number = {9}, + journal = {The Physics of Fluids}, + author = {Chodura, R}, + month = sep, + year = {1982}, + note = {Publisher: American Institute of Physics}, + keywords = {\_tablet}, + pages = {1628--1633}, + file = {Chodura_1982_Plasma{\textendash}wall transition in an oblique magnetic field.pdf:/home/ym266336/Zotero/storage/IBMAQQFR/Chodura_1982_Plasma{\textendash}wall transition in an oblique magnetic field.pdf:application/pdf}, +} + +@article{Esteve2015, + title = {A multi-species collisional operator for full-{F} gyrokinetics}, + volume = {22}, + issn = {1070-664X}, + url = {https://doi.org/10.1063/1.4937373}, + doi = {10.1063/1.4937373}, + number = {12}, + journal = {Physics of Plasmas}, + author = {Est{\`e}ve, D and Garbet, X and Sarazin, Y and Grandgirard, V and Cartier-Michaud, T and Dif-Pradalier, G and Ghendrih, P and Latu, G and Norscini, C}, + month = dec, + year = {2015}, + note = {Publisher: American Institute of Physics}, + keywords = {\_tablet}, + pages = {122506}, + file = {Est{\`e}ve et al_2015_A multi-species collisional operator for full-F gyrokinetics.pdf:/home/ym266336/Zotero/storage/L6EBU9M3/Est{\`e}ve et al_2015_A multi-species collisional operator for full-F gyrokinetics.pdf:application/pdf}, +} + +@article{Moyer1995, + title = {Beyond paradigm: {Turbulence}, transport, and the origin of the radial electric field in low to high confinement mode transitions in the {DIII}-{D} tokamak}, + volume = {2}, + issn = {1070-664X}, + url = {https://doi.org/10.1063/1.871263}, + doi = {10.1063/1.871263}, + number = {6}, + journal = {Physics of Plasmas}, + author = {Moyer, R A and Burrell, K H and Carlstrom, T N and Coda, S and Conn, R W and Doyle, E J and Gohil, P and Groebner, R J and Kim, J and Lehmer, R and Peebles, W A and Porkolab, M and Rettig, C L and Rhodes, T L and Seraydarian, R P and Stockdale, R and Thomas, D M and Tynan, G R and Watkins, J G}, + month = jun, + year = {1995}, + note = {Publisher: American Institute of Physics}, + keywords = {\_tablet}, + pages = {2397--2407}, + file = {Moyer et al_1995_Beyond paradigm.pdf:/home/ym266336/Zotero/storage/J9YNP8HP/Moyer et al_1995_Beyond paradigm.pdf:application/pdf}, +} + +@article{Verboncoeur1993, + title = {Simultaneous {Potential} and {Circuit} {Solution} for {1D} {Bounded} {Plasma} {Particle} {Simulation} {Codes}}, + volume = {104}, + issn = {0021-9991}, + url = {https://www.sciencedirect.com/science/article/pii/S002199918371034X}, + doi = {https://doi.org/10.1006/jcph.1993.1034}, + abstract = {A general second-order accurate method for solving the combined potential and circuit equations in a one-dimensional electrostatic bounded plasma PIC simulation is presented. The boundary conditions include surface charge on the electrodes, which are connected to a series RLC circuit with driving terms V (t) or I(t). The solution is obtained for planer, cylindrical, and spherical electrodes. The results is a tridiagonal matrix which is readily solved using well-known methods. The methods is implemented in the codes PDP1 (plasma device planar 1D), PDC1 (cylindrical), and PDS1 (spherical).}, + number = {2}, + journal = {Journal of Computational Physics}, + author = {Verboncoeur, J P and Alves, M V and Vahedi, V and Birdsall, C K}, + year = {1993}, + keywords = {\_tablet}, + pages = {321--328}, + file = {Verboncoeur et al_1993_Simultaneous Potential and Circuit Solution for 1D Bounded Plasma Particle.pdf:/home/ym266336/Zotero/storage/ERPP9SS6/Verboncoeur et al_1993_Simultaneous Potential and Circuit Solution for 1D Bounded Plasma Particle.pdf:application/pdf}, +} + +@article{Dif-Pradalier2011, + title = {Neoclassical physics in full distribution function gyrokinetics}, + volume = {18}, + issn = {1070-664X}, + url = {https://doi.org/10.1063/1.3592652}, + doi = {10.1063/1.3592652}, + number = {6}, + journal = {Physics of Plasmas}, + author = {Dif-Pradalier, G and Diamond, P H and Grandgirard, V and Sarazin, Y and Abiteboul, J and Garbet, X and Ghendrih, Ph. and Latu, G and Strugarek, A and Ku, S and Chang, C S}, + month = jun, + year = {2011}, + note = {Publisher: American Institute of Physics}, + keywords = {\_tablet}, + pages = {62309}, + file = {Dif-Pradalier et al_2011_Neoclassical physics in full distribution function gyrokinetics.pdf:/home/ym266336/Zotero/storage/8FPLPEIB/Dif-Pradalier et al_2011_Neoclassical physics in full distribution function gyrokinetics.pdf:application/pdf}, +} + +@article{Escande2021, + title = {Plasma-wall self-organization in magnetic fusion}, + volume = {62}, + issn = {0029-5515}, + url = {http://dx.doi.org/10.1088/1741-4326/ac3c87}, + doi = {10.1088/1741-4326/ac3c87}, + abstract = {This paper introduces the concept of plasma-wall self-organization (PWSO) in magnetic fusion. The basic idea is the existence of a time delay in the feedback loop relating radiation and impurity production on divertor plates. Both a zero and a one-dimensional description of PWSO are provided. They lead to an iterative equation whose equilibrium fixed point~is unstable above some threshold. This threshold corresponds to a radiative density limit, which can be reached for a ratio of total radiated power to total input power as low as 1/2. When detachment develops and physical sputtering dominates, this limit is progressively pushed to very high values if the radiation of non-plate impurities stays low. Therefore, PWSO comes with two basins for this organization: the usual one with a density limit, and a new one with density freedom, in particular for machines using high-Z materials. Two basins of attraction of PWSO are shown to exist for the tokamak during start-up, with a high density one leading to this freedom. This basin~might be reached by a proper tailoring of ECRH assisted ohmic start-up in present middle-size tokamaks, mimicking present stellarator start-up. In view of the impressive tokamak DEMO wall load challenge, it is worth considering and checking this possibility, which comes with that of more margins for ITER and of smaller reactors.}, + number = {2}, + journal = {Nuclear Fusion}, + author = {Escande, D F and Sattin, F and Zanca, P}, + year = {2021}, + note = {Publisher: IOP Publishing}, + pages = {26001}, +} + +@article{Shi2015, + title = {A gyrokinetic one-dimensional scrape-off layer model of an edge-localized mode heat pulse}, + volume = {22}, + issn = {1070-664X}, + url = {https://doi.org/10.1063/1.4907160}, + doi = {10.1063/1.4907160}, + number = {2}, + journal = {Physics of Plasmas}, + author = {Shi, E L and Hakim, A H and Hammett, G W}, + month = feb, + year = {2015}, + note = {Publisher: American Institute of Physics}, + keywords = {\_tablet}, + pages = {22504}, + file = {Shi et al_2015_A gyrokinetic one-dimensional scrape-off layer model of an edge-localized mode.pdf:/home/ym266336/Zotero/storage/WDMKKLJG/Shi et al_2015_A gyrokinetic one-dimensional scrape-off layer model of an edge-localized mode.pdf:application/pdf}, +} + +@book{Stangeby, + title = {The {Plasma} {Boundary} of {Magnetic} {Fusion} {Devices}}, + author = {Stangeby, P C}, + year = {2000}, +} + +@article{Donnel_2020, + title = {Moment approach of the multi-species non-linear {Coulomb} collision operator adapted to particle-in-cell codes}, + volume = {63}, + url = {https://doi.org/10.1088/1361-6587/abc92b}, + doi = {10.1088/1361-6587/abc92b}, + abstract = {In this article an approximated version of the multi-species, non-linear Coulomb collision operator is derived via the use of a truncated moment expansion of the distribution function to compute the Rosenbluth potentials. The evolution of the distribution function due to the collision operator takes the form of a Fokker{\textendash}Planck equation that can be efficiently solved by a Langevin approach in the particle-in-cell (PIC) framework. This kinetic collision operator is then implemented in the global gyrokinetic PIC code ORB5 while neglecting finite Larmor effects. This collision operator ensures exact conservation of density, total momentum and energy as expected. The neoclassical physics is also successfully retrieved by the code. Numerical aspects such as the noise control and the parallelisation of the code are presented in detail.}, + number = {2}, + journal = {Plasma Physics and Controlled Fusion}, + author = {Donnel, P and Gheller, C and Brunner, S and Villard, L and Lanti, E and Ohana, N and Murugappan, M}, + year = {2020}, + note = {Publisher: \{IOP\} Publishing}, + keywords = {\_tablet}, + pages = {25006}, + file = {Donnel et al_2020_Moment approach of the multi-species non-linear Coulomb collision operator.pdf:/home/ym266336/Zotero/storage/5YQ4QF4V/Donnel et al_2020_Moment approach of the multi-species non-linear Coulomb collision operator.pdf:application/pdf}, +} + +@article{Grandgirard2016, + title = {A {5D} gyrokinetic full-f global semi-{Lagrangian} code for flux-driven ion turbulence simulations}, + volume = {207}, + issn = {0010-4655}, + url = {https://www.sciencedirect.com/science/article/pii/S0010465516301230}, + doi = {https://doi.org/10.1016/j.cpc.2016.05.007}, + journal = {Computer Physics Communications}, + author = {Grandgirard, V and Abiteboul, J and Bigot, J and Cartier-Michaud, T and Crouseilles, N and Dif-Pradalier, G and Ehrlacher, Ch. and Esteve, D and Garbet, X and Ghendrih, Ph. and Latu, G and Mehrenberger, M and Norscini, C and Passeron, Ch. and Rozar, F and Sarazin, Y and Sonnendr{\"u}cker, E and Strugarek, A and Zarzoso, D}, + year = {2016}, + keywords = {Gyrokinetic global full-f flux-driven simulations, High-performance computing, Plasma turbulence, Semi-Lagrangian method, \_tablet}, + pages = {35--68}, + file = {Grandgirard et al_2016_A 5D gyrokinetic full-f global semi-Lagrangian code for flux-driven ion.pdf:/home/ym266336/Zotero/storage/QLLDRX5B/Grandgirard et al_2016_A 5D gyrokinetic full-f global semi-Lagrangian code for flux-driven ion.pdf:application/pdf}, +} + +@inproceedings{Donnel2022, + title = {Impact of the transition from open to closed field lines on turbulent transport in tokamaks}, + author = {Donnel, Peter and Dif-pradalier, Guilhem and Giannatale, Giovanni Di and Villard, Laurent and Grandgirard, Virginie and Nguyen, Laurent and Sarazin, Yanick and Varennes, Robin}, + year = {2022}, + keywords = {\_tablet}, + pages = {12006}, + file = {Donnel et al_2022_Impact of the transition from open to closed field lines on turbulent transport.pdf:/home/ym266336/Zotero/storage/GS2JUKCR/Donnel et al_2022_Impact of the transition from open to closed field lines on turbulent transport.pdf:application/pdf}, +} + +@article{Pan2016, + title = {Fully nonlinear $\delta$f gyrokinetics for scrape-off layer parallel transport}, + volume = {23}, + issn = {1070-664X}, + url = {https://doi.org/10.1063/1.4964666}, + doi = {10.1063/1.4964666}, + number = {10}, + journal = {Physics of Plasmas}, + author = {Pan, Q and Told, D and Jenko, F}, + month = oct, + year = {2016}, + note = {Publisher: American Institute of Physics}, + keywords = {\_tablet}, + pages = {102302}, + file = {Pan et al_2016_Fully nonlinear $\delta$f gyrokinetics for scrape-off layer parallel transport.pdf:/home/ym266336/Zotero/storage/E3RZWJIF/Pan et al_2016_Fully nonlinear $\delta$f gyrokinetics for scrape-off layer parallel transport.pdf:application/pdf}, +} + +@article{Burrell1997, + title = {Effects of {E}{\texttimes}{B} velocity shear and magnetic shear on turbulence and transport in magnetic confinement devices}, + volume = {4}, + issn = {1070-664X}, + url = {https://doi.org/10.1063/1.872367}, + doi = {10.1063/1.872367}, + number = {5}, + journal = {Physics of Plasmas}, + author = {Burrell, K H}, + month = may, + year = {1997}, + note = {Publisher: American Institute of Physics}, + keywords = {\_tablet}, + pages = {1499--1518}, + file = {Burrell_1997_Effects of E{\texttimes}B velocity shear and magnetic shear on turbulence and transport in.pdf:/home/ym266336/Zotero/storage/PKB6V4KF/Burrell_1997_Effects of E{\texttimes}B velocity shear and magnetic shear on turbulence and transport in.pdf:application/pdf}, +} + +@misc{bourne:cea-03748016, + title = {Non-{Uniform} {Splines} for {Semi}-{Lagrangian} {Kinetic} {Simulations} of the {Plasma} {Sheath}}, + url = {https://hal-cea.archives-ouvertes.fr/cea-03748016}, + author = {Bourne, Emily and Munschy, Yann and Grandgirard, Virginie and Mehrenberger, Michel and Ghendrih, Philippe}, + year = {2022}, + keywords = {\_tablet}, + file = {Bourne et al_2022_Non-Uniform Splines for Semi-Lagrangian Kinetic Simulations of the Plasma Sheath.pdf:/home/ym266336/Zotero/storage/6B55ZC7U/Bourne et al_2022_Non-Uniform Splines for Semi-Lagrangian Kinetic Simulations of the Plasma Sheath.pdf:application/pdf}, +} + +@article{Caschera_2018, + title = {Immersed boundary conditions in global, flux-driven, gyrokinetic simulations}, + volume = {1125}, + url = {https://doi.org/10.1088/1742-6596/1125/1/012006}, + doi = {10.1088/1742-6596/1125/1/012006}, + abstract = {A penalization technique is applied in global and flux driven gyrokinetic simulations to model a limiter configuration. The immersed boundary is implemented in terms of a restoring force to a cold distribution function. It acts as a perfect heat absorber. Parallel kinetic propagation of a cold front generated by the limiter is tested with a 1-D 1-V single species model. An analytical expression is derived to describe the initial transient of the density, particle flux and energy profiles, induced by the ballistic propagation of the cold front in phase space(x, v). The same propagation is recovered in the global gyrokinetic code on the distribution function along the poloidal direction. The velocity of the front measured in the code matches the theoretical prediction.}, + journal = {Journal of Physics: Conference Series}, + author = {Caschera, E and Dif-Pradalier, G and Ghendrih, Ph. and Grandgirard, V and Asahi, Y and Bouzat, N and Donnel, P and Garbet, X and Latu, G and Passeron, C and Sarazin, Y}, + month = nov, + year = {2018}, + note = {Publisher: \{IOP\} Publishing}, + keywords = {\_tablet}, + pages = {12006}, + file = {Caschera et al_2018_Immersed boundary conditions in global, flux-driven, gyrokinetic simulations.pdf:/home/ym266336/Zotero/storage/9IDUT3ST/Caschera et al_2018_Immersed boundary conditions in global, flux-driven, gyrokinetic simulations.pdf:application/pdf}, +} + +@article{Wagner_2007, + title = {A quarter-century of {H}-mode studies}, + volume = {49}, + url = {https://doi.org/10.1088/0741-3335/49/12b/s01}, + doi = {10.1088/0741-3335/49/12b/s01}, + abstract = {The H-mode is a confinement mode of toroidal plasmas, which may make the goals of fusion possible{\textemdash}the development of a clean energy source at competitive electricity costs. The most challenging aspect of the H-mode physics is the sudden disappearance of the edge turbulence whereas its driving forces{\textemdash}the gradients{\textemdash}increase. As the physics behind the H-mode is subtle many features are not yet clarified. There is, however, substantial experimental and theoretical evidence that turbulent flows, which normally limit the confinement, are diminished by sheared poloidal flow residing at the plasma edge. There are many conceivable mechanisms giving rise to sheared flow. The most intriguing of these is that fluctuations themselves induce the flow, which acts back to its generating origin and annihilates the turbulence. This review concentrates mostly on the transition physics, describes one line of understanding the H-mode in more detail, recalls some of the older observations and summarizes the achievements in the H-mode for both tokamaks and stellarators.}, + number = {12B}, + journal = {Plasma Physics and Controlled Fusion}, + author = {Wagner, F}, + month = nov, + year = {2007}, + note = {Publisher: \{IOP\} Publishing}, + keywords = {\_tablet}, + pages = {B1--B33}, + file = {Wagner_2007_A quarter-century of H-mode studies.pdf:/home/ym266336/Zotero/storage/K896U53Z/Wagner_2007_A quarter-century of H-mode studies.pdf:application/pdf;Wagner_2007_A quarter-century of H-mode studies.pdf:/home/ym266336/Zotero/storage/J4IDU78Q/Wagner_2007_A quarter-century of H-mode studies.pdf:application/pdf}, +} + +@article{Moulton2013, + title = {Quasineutral plasma expansion into infinite vacuum as a model for parallel {ELM} transport}, + volume = {55}, + issn = {0741-3335}, + url = {http://dx.doi.org/10.1088/0741-3335/55/8/085003}, + doi = {10.1088/0741-3335/55/8/085003}, + abstract = {An analytic solution for the expansion of a plasma into vacuum is assessed for its relevance to the parallel transport of edge localized mode (ELM) filaments along field lines. This solution solves the 1D1V Vlasov{\textendash}Poisson equations for the adiabatic (instantaneous source), collisionless expansion of a Gaussian plasma bunch into an infinite space in the quasineutral limit. The quasineutral assumption is found to hold as long as $\lambda$D0/$\sigma$0 ? 0.01 (where $\lambda$D0 is the initial Debye length at peak density and $\sigma$0 is the parallel length of the Gaussian filament), a condition that is physically realistic. The inclusion of a boundary at x = L and consequent formation of a target sheath is found to have a negligible effect when L/$\sigma$0 ? 5, a condition that is physically plausible. Under the same condition, the target flux densities predicted by the analytic solution are well approximated by the {\textquoteleft}free-streaming{\textquoteright} equations used in previous experimental studies, strengthening the notion that these simple equations are physically reasonable. Importantly, the analytic solution predicts a zero heat flux density so that a fluid approach to the problem can be used equally well, at least when the source is instantaneous. It is found that, even for JET-like pedestal parameters, collisions can affect the expansion dynamics via electron temperature isotropization, although this is probably a secondary effect. Finally, the effect of a finite duration, $\tau$src, for the plasma source is investigated. As is found for an instantaneous source, when L/$\sigma$0 ? 5 the presence of a target sheath has a negligible effect, at least up to the explored range of $\tau$src = L/cs (where cs is the sound speed at the initial temperature).}, + number = {8}, + journal = {Plasma Physics and Controlled Fusion}, + author = {Moulton, D and Ghendrih, Ph and Fundamenski, W and Manfredi, G and Tskhakaya, D}, + year = {2013}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {85003}, + file = {Moulton et al_2013_Quasineutral plasma expansion into infinite vacuum as a model for parallel ELM.pdf:/home/ym266336/Zotero/storage/FYBUGNKM/Moulton et al_2013_Quasineutral plasma expansion into infinite vacuum as a model for parallel ELM.pdf:application/pdf}, +} + +@article{langmuir_interaction_1929, + title = {The {Interaction} of {Electron} and {Positive} {Ion} {Space} {Charges} in {Cathode} {Sheaths}}, + volume = {33}, + url = {https://link.aps.org/doi/10.1103/PhysRev.33.954}, + doi = {10.1103/PhysRev.33.954}, + number = {6}, + journal = {Phys. Rev.}, + author = {Langmuir, Irving}, + month = jun, + year = {1929}, + note = {Publisher: American Physical Society}, + keywords = {\_tablet}, + pages = {954--989}, + file = {Langmuir_1929_The Interaction of Electron and Positive Ion Space Charges in Cathode Sheaths.pdf:/home/ym266336/Zotero/storage/5WK3NVGX/Langmuir_1929_The Interaction of Electron and Positive Ion Space Charges in Cathode Sheaths.pdf:application/pdf}, +} + +@article{tonks_general_1929, + title = {A {General} {Theory} of the {Plasma} of an {Arc}}, + volume = {34}, + url = {https://link.aps.org/doi/10.1103/PhysRev.34.876}, + doi = {10.1103/PhysRev.34.876}, + number = {6}, + journal = {Phys. Rev.}, + author = {Tonks, Lewi and Langmuir, Irving}, + month = sep, + year = {1929}, + note = {Publisher: American Physical Society}, + keywords = {\_tablet}, + pages = {876--922}, + file = {Tonks_Langmuir_1929_A General Theory of the Plasma of an Arc.pdf:/home/ym266336/Zotero/storage/4TYG7NM4/Tonks_Langmuir_1929_A General Theory of the Plasma of an Arc.pdf:application/pdf}, +} + +@incollection{Bohm1949, + address = {ch 3, p 77}, + edition = {A. Guthry and R. K .Wakerling (New York: MacGraw-Hill)}, + title = {The {Characteristics} of {Electrical} {Discharges} in {Magnetic} {Fields}}, + booktitle = {The {Characteristics} of {Electrical} {Discharges} in {Magnetic} {Fields}}, + author = {Bohm, David}, + year = {1949}, + keywords = {\_tablet}, + file = {Bohm_1949_The Characteristics of Electrical Discharges in Magnetic Fields.pdf:/home/ym266336/Zotero/storage/85EZ3U4C/Bohm_1949_The Characteristics of Electrical Discharges in Magnetic Fields.pdf:application/pdf}, +} + +@article{harrison_low_1959, + title = {The {Low} {Pressure} {Plane} {Symmetric} {Discharge}}, + volume = {74}, + url = {https://doi.org/10.1088/0370-1328/74/2/301}, + doi = {10.1088/0370-1328/74/2/301}, + abstract = {It is shown that the low pressure plane symmetric plasma equation, using the collision-free model of Tonks and Langmuir, can be solved analytically. Simple expressions are obtained for the mean velocity and the mean square velocity of the ions, and for the wall potential with respect to the plasma. The conditions for the formation of a stable plasma-sheath boundary are briefly examined and a general criterion is obtained without considering any specific mechanism of ion transport. No assumptions are made regarding the energy distribution of the ions, and the result is therefore a refinement on Bohm's original criterion which was derived by assuming a monoenergetic ion flux. With the aid of the criterion developed in the present treatment conclusions are then drawn in the case of the collision-free model regarding conditions applying at the plasma boundary. The experimental results are found to be consistent with these theoretical conditions.}, + number = {2}, + journal = {Proceedings of the Physical Society}, + author = {Harrison, E. R. and Thompson, W. B.}, + month = aug, + year = {1959}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {145--152}, + file = {Harrison_Thompson_1959_The Low Pressure Plane Symmetric Discharge.pdf:/home/ym266336/Zotero/storage/C2MNS6JF/Harrison_Thompson_1959_The Low Pressure Plane Symmetric Discharge.pdf:application/pdf}, +} + +@article{boyd_mechanism_1951, + title = {The {Mechanism} of {Positive} {Ion} {Collection} by a {Spherical} {Probe} in a {Dense} {Gas}}, + volume = {64}, + url = {https://doi.org/10.1088/0370-1301/64/9/311}, + doi = {10.1088/0370-1301/64/9/311}, + abstract = {The Langmuir probe technique is not suitable for measuring ion densities above 1 mm Hg pressure because the probe dimensions approach those of the ionic and electronic mean free paths. In addition to the invalidity of the Langmuir theory for this case, such a probe also causes a great disturbance of the discharge. In this paper a detailed examination is made of the possibility of using a probe collecting positive ions as a means of finding ion densities It has been found possible to calculate the potential distribution, outside a space-charge sheath around a spherical probe, if the radius of the sheath is known From this the current of positive ions to the probe may be found Curves are given to facilitate this calculation. It is found that, depending on the ion concentration and pressure, there are two rather different sets of conditions around the probe. If the ion density is high (greater than about 108/mean free path (in cm)) a thin sheath will form on the probe and a complete solution of the problem is possible Under such conditions the energies of the diffusing ions in the neighbourhood of the probe greatly exceed the thermal energies of the gas particles At the lower ion densities normally encountered, a thick `diffusion' sheath occurs and the problem can now only be solved if the sheath thickness is known The ion energies may or may not greatly exceed the thermal energies, depending on conditions. These results contradict one of the basic assumptions made by Davydov and Zmanovskaja in their approach to the same problem They assume a thin sheath with the ions in thermal equilibrium with the surrounding gas As a result their conclusion is in conflict with the conclusion of this paper, that in most circumstances it is not possible to use a negative probe to measure ion densities unless an additional means of determining the sheath thickness is available.}, + number = {9}, + journal = {Proceedings of the Physical Society. Section B}, + author = {Boyd, R. L. F.}, + month = sep, + year = {1951}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {795--804}, + file = {Boyd_1951_The Mechanism of Positive Ion Collection by a Spherical Probe in a Dense Gas.pdf:/home/ym266336/Zotero/storage/SF2T75EJ/Boyd_1951_The Mechanism of Positive Ion Collection by a Spherical Probe in a Dense Gas.pdf:application/pdf}, +} + +@article{persson_inertiacontrolled_1962, + title = {Inertia-{Controlled} {Ambipolar} {Diffusion}}, + volume = {5}, + url = {https://aip.scitation.org/doi/abs/10.1063/1.1706574}, + doi = {10.1063/1.1706574}, + number = {12}, + journal = {The Physics of Fluids}, + author = {Persson, Karl-Birger}, + year = {1962}, + note = {\_eprint: https://aip.scitation.org/doi/pdf/10.1063/1.1706574}, + keywords = {\_tablet}, + pages = {1625--1632}, + file = {Persson_1962_Inertia-Controlled Ambipolar Diffusion.pdf:/home/ym266336/Zotero/storage/BYB7HRDW/Persson_1962_Inertia-Controlled Ambipolar Diffusion.pdf:application/pdf}, +} + +@article{riemann_kinetic_1981, + title = {Kinetic theory of the plasma sheath transition in a weakly ionized plasma}, + volume = {24}, + url = {https://aip.scitation.org/doi/abs/10.1063/1.863332}, + doi = {10.1063/1.863332}, + number = {12}, + journal = {The Physics of Fluids}, + author = {Riemann, K.-U.}, + year = {1981}, + note = {\_eprint: https://aip.scitation.org/doi/pdf/10.1063/1.863332}, + keywords = {\_tablet}, + pages = {2163--2172}, + file = {Riemann_1981_Kinetic theory of the plasma sheath transition in a weakly ionized plasma.pdf:/home/ym266336/Zotero/storage/4RN2CX9U/Riemann_1981_Kinetic theory of the plasma sheath transition in a weakly ionized plasma.pdf:application/pdf}, +} + +@article{stangeby_plasma_1970, + title = {Plasma boundary as a {Mach} surface}, + volume = {3}, + url = {https://doi.org/10.1088/0305-4470/3/3/017}, + doi = {10.1088/0305-4470/3/3/017}, + abstract = {Ion motion in a plasma is treated by the equations of compressible fluid flow. The plasma-sheath boundary is identified as a closed Mach surface thus demonstrating that the Bohm criterion applies to the component of ion velocity normal to the sheath edge.}, + number = {3}, + journal = {Journal of Physics A: General Physics}, + author = {Stangeby, P. C. and Allen, J. E.}, + month = may, + year = {1970}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {304--308}, + file = {Stangeby_Allen_1970_Plasma boundary as a Mach surface.pdf:/home/ym266336/Zotero/storage/S89GQWW6/Stangeby_Allen_1970_Plasma boundary as a Mach surface.pdf:application/pdf}, +} + +@article{moritz_plasma-wall_2019, + title = {The plasma-wall transition with collisions and an oblique magnetic field: reversal of potential drops at grazing incidences}, + volume = {26}, + url = {https://hal.archives-ouvertes.fr/hal-02171905}, + doi = {10.1063/1.5061832}, + number = {1}, + journal = {Physics of Plasmas}, + author = {Moritz, J. and Lesur, Maxime and Faudot, E. and Devaux, S. and Heuraux, S. and Ledig, J.}, + year = {2019}, + note = {Publisher: American Institute of Physics}, + keywords = {PIC simulations, \_tablet, 5240Fd Keywords: Plasma sheath, 5265Rr, Magnetic confinement, numbers: 5240Kh}, + pages = {013507}, + file = {Moritz et al_2019_The plasma-wall transition with collisions and an oblique magnetic field.pdf:/home/ym266336/Zotero/storage/UJ5XYCGV/Moritz et al_2019_The plasma-wall transition with collisions and an oblique magnetic field.pdf:application/pdf}, +} + +@article{hu_collisionless_1968, + title = {Collisionless {Plasma} {Sheath} with {Transverse} {Flow}}, + volume = {11}, + url = {https://aip.scitation.org/doi/abs/10.1063/1.1691931}, + doi = {10.1063/1.1691931}, + number = {2}, + journal = {The Physics of Fluids}, + author = {Hu, Pung Nien and Ziering, Sigi}, + year = {1968}, + note = {\_eprint: https://aip.scitation.org/doi/pdf/10.1063/1.1691931}, + keywords = {\_tablet}, + pages = {451--453}, + file = {Hu_Ziering_1968_Collisionless Plasma Sheath with Transverse Flow.pdf:/home/ym266336/Zotero/storage/SSVQWLI6/Hu_Ziering_1968_Collisionless Plasma Sheath with Transverse Flow.pdf:application/pdf}, +} + +@article{robertson_sheaths_2013, + title = {Sheaths in laboratory and space plasmas}, + volume = {55}, + doi = {10.1088/0741-3335/55/9/093001}, + number = {9}, + journal = {Plasma Physics and Controlled Fusion}, + author = {Robertson, Scott}, + month = sep, + year = {2013}, + keywords = {\_tablet}, + pages = {093001}, + file = {Robertson_2013_Sheaths in laboratory and space plasmas.pdf:/home/ym266336/Zotero/storage/IGQF47TU/Robertson_2013_Sheaths in laboratory and space plasmas.pdf:application/pdf}, +} + +@misc{dif-pradalier_transport_2022, + title = {Transport in fusion plasmas: is the tail wagging the dog?}, + copyright = {Creative Commons Attribution 4.0 International}, + url = {https://arxiv.org/abs/2206.04193}, + publisher = {arXiv}, + author = {Dif-Pradalier, Guilhem and Ghendrih, Philippe and Sarazin, Yanick and Camenen, Yann and Donnel, Peter and Garbet, Xavier and Grandgirard, Virginie and Munschy, Yann and Vermare, Laure and Widmer, Fabien}, + year = {2022}, + doi = {10.48550/ARXIV.2206.04193}, + keywords = {\_tablet, FOS: Physical sciences, Plasma Physics (physics.plasm-ph)}, + file = {Dif-Pradalier et al_2022_Transport in fusion plasmas.pdf:/home/ym266336/Zotero/storage/DBB9XQ6M/Dif-Pradalier et al_2022_Transport in fusion plasmas.pdf:application/pdf}, +} + +@article{bufferand_numerical_2015, + title = {Numerical modelling for divertor design of the {WEST} device with a focus on plasma{\textendash}wall interactions}, + volume = {55}, + url = {https://doi.org/10.1088/0029-5515/55/5/053025}, + doi = {10.1088/0029-5515/55/5/053025}, + abstract = {In the perspective of operating tungsten monoblocks in WEST, the ongoing major upgrade of the Tore Supra tokamak, a dedicated modelling effort has been carried out to simulate the interaction between the edge plasma and the tungsten wall. A new transport code, SolEdge2D{\textendash}EIRENE, has been developed with the ability to simulate the plasma up to the first wall. This is especially important for steady state operation, where thermal loads on all the plasma facing components, even remote from the plasma, are of interest. Moreover, main chamber tungsten sources are thought to dominate the contamination of the plasma core. We present here in particular new developments aimed at improving the description of the interface between the plasma and the wall, namely a way to treat sheath physics in a more faithful way using the output of 1D particle in cell simulations. Moreover, different models for prompt redeposition have been implemented and are compared. The latter is shown to play an important role in the balance between divertor and main chamber sources.}, + number = {5}, + journal = {Nuclear Fusion}, + author = {Bufferand, H. and Ciraolo, G. and Marandet, Y. and Bucalossi, J. and Ghendrih, Ph and Gunn, J. and Mellet, N. and Tamain, P. and Leybros, R. and Fedorczak, N. and Schwander, F. and Serre, E.}, + month = apr, + year = {2015}, + note = {Publisher: IOP Publishing}, + keywords = {\_tablet}, + pages = {053025}, + file = {Bufferand et al_2015_Numerical modelling for divertor design of the WEST device with a focus on.pdf:/home/ym266336/Zotero/storage/2ZUP7CTK/Bufferand et al_2015_Numerical modelling for divertor design of the WEST device with a focus on.pdf:application/pdf}, +} + +@article{bufferand_near_2013, + title = {Near wall plasma simulation using penalization technique with the transport code {SolEdge2D}-{Eirene}}, + volume = {438}, + issn = {0022-3115}, + url = {https://www.sciencedirect.com/science/article/pii/S0022311513000986}, + doi = {https://doi.org/10.1016/j.jnucmat.2013.01.090}, + abstract = {In order to model plasma interaction with full complexity of the geometry of PFCs, an immersed method to impose boundary conditions has been implemented in the transport code SolEdge2D. This penalization technique has proven to properly recover Bohm boundary conditions, including supersonic solutions at the sheath entrance. The role of the ionization source has been taken into account by coupling SolEdge2D with the 3D kinetic neutral code Eirene. Density regimes are properly recovered and major differences between core located and divertor located ionization source regimes are emphasized. One also presents main chamber wall recycling regime simulations that can now be addressed with simulations of the entire edge plasma up to the wall.}, + journal = {Journal of Nuclear Materials}, + author = {Bufferand, H. and Bensiali, B. and Bucalossi, J. and Ciraolo, G. and Genesio, P. and Ghendrih, Ph and Marandet, Y. and Paredes, A. and Schwander, F. and Serre, E. and Tamain, P.}, + year = {2013}, + keywords = {\_tablet}, + pages = {S445--S448}, + file = {Bufferand et al_2013_Near wall plasma simulation using penalization technique with the transport.pdf:/home/ym266336/Zotero/storage/U74J5N7U/Bufferand et al_2013_Near wall plasma simulation using penalization technique with the transport.pdf:application/pdf}, +} + +@article{isoardi_penalization_2010, + title = {Penalization modeling of a limiter in the {Tokamak} edge plasma}, + volume = {229}, + doi = {10.1016/j.jcp.2009.11.031}, + journal = {Journal of Computational Physics}, + author = {Isoardi, Livia and Chiavassa, Guillaume and Ciraolo, G. and Haldenwang, Pierre and Serre, Eric and Ghendrih, Ph and Sarazin, Yanick and Schwander, Frederic and Tamain, Patrick}, + month = mar, + year = {2010}, + pages = {2220--2235}, +} + +@article{dif-pradalier_transport_2022-1, + title = {Transport barrier onset and edge turbulence shortfall in fusion plasmas}, + volume = {5}, + issn = {2399-3650}, + url = {https://doi.org/10.1038/s42005-022-01004-z}, + doi = {10.1038/s42005-022-01004-z}, + abstract = {Magnetic confinement fusion offers the promise of sustainable and safe energy production on Earth. Advanced experimental scenarios exploit the fascinating yet uncommon ability of confined plasmas to bifurcate into states of enhanced performance upon application of additional free energy sources. Self-regulation of small-scale turbulent eddies is essential to accessing these improved regimes. However, after several decades, basic principles for these bifurcations are still largely debated and clarifications from first principles lacking. We show here, computed from the primitive kinetic equations, establishment of a state of improved confinement through self-organisation of plasma microturbulence. Our results highlight the critical role of the interface between plasma and material boundaries and demonstrate the importance of propagation of turbulence activity beyond regions of convective drive. These observations strongly suggest a paradigm shift where the magnetised plasma at the onset of enhanced performance self-organises into a globally critical state, {\textquoteleft}nonlocally{\textquoteright} controlled by fluxes of turbulence activity.}, + number = {1}, + journal = {Communications Physics}, + author = {Dif-Pradalier, Guilhem and Ghendrih, Philippe and Sarazin, Yanick and Caschera, Elisabetta and Clairet, Fr{\'e}d{\'e}ric and Camenen, Yann and Donnel, Peter and Garbet, Xavier and Grandgirard, Virginie and Munschy, Yann and Vermare, Laure and Widmer, Fabien}, + month = sep, + year = {2022}, + pages = {229}, +} + +@article{korpilo_gyrokinetic_2016, + title = {Gyrokinetic full-torus simulations of ohmic tokamak plasmas in circular limiter configuration}, + volume = {203}, + doi = {10.1016/j.cpc.2016.02.021}, + journal = {Computer Physics Communications}, + author = {Korpilo, T. and Gurchenko, A.D. and Gusakov, E. and Heikkinen, J.A. and Janhunen, Salomon and Kiviniemi, T.P. and Leerink, S. and Niskala, Paavo and Perevalov, Artur}, + month = mar, + year = {2016}, +} + +@article{chang_gyrokinetic_2017, + title = {Gyrokinetic projection of the divertor heat-flux width from present tokamaks to {ITER}}, + volume = {57}, + issn = {0029-5515}, + url = {http://dx.doi.org/10.1088/1741-4326/aa7efb}, + doi = {10.1088/1741-4326/aa7efb}, + abstract = {The XGC1 edge gyrokinetic code is used to study the width of the heat-flux to divertor plates in attached plasma condition. The flux-driven simulation is performed until an approximate power balance is achieved between the heat-flux across the steep pedestal pressure gradient and the heat-flux on the divertor plates. The simulation results compare well against the empirical scaling $\lambda$ q 1/ obtained from present tokamak devices, where $\lambda$ q is the divertor heat-flux width mapped to the outboard midplane, $\gamma$ = 1.19 as found by Eich et al (2013 Nucl. Fusion 53 093031), and B P is the magnitude of the poloidal magnetic field at the outboard midplane separatrix surface. This empirical scaling predicts $\lambda$ q ? 1 mm when extrapolated to ITER, which would require operation with very high separatrix densities (n sep/n Greenwald {\textgreater} 0.6) (Kukushkin et al 2013 J. Nucl. Mater. 438 S203) in the Q = 10 scenario to achieve semi-detached plasma operation and high radiative fractions for acceptable divertor power fluxes. Using the same simulation code and technique, however, the projected $\lambda$ q for ITER{\textquoteright}s model plasma is 5.9 mm, which could be suggesting that operation in the ITER Q = 10 scenario with acceptable divertor power loads may be obtained over a wider range of plasma separatrix densities and radiative fractions. The physics reason behind this difference is, according to the XGC1 results, that while the ion magnetic drift contribution to the divertor heat-flux width is wider in the present tokamaks, the turbulent electron contribution is wider in ITER. Study will continue to verify further this important projection. A high current C-Mod discharge is found to be in a mixed regime: While the heat-flux width by the ion neoclassical magnetic drift is still wider than the turbulent electron heat-flux width, the heat-flux magnitude is dominated by the narrower electron heat-flux.}, + number = {11}, + journal = {Nuclear Fusion}, + author = {Chang, C.S. and Ku, S. and Loarte, A. and Parail, V. and K{\"o}chl, F. and Romanelli, M. and Maingi, R. and Ahn, J.-W. and Gray, T. and Hughes, J. and LaBombard, B. and Leonard, T. and Makowski, M. and Terry, J.}, + month = aug, + year = {2017}, + note = {Publisher: IOP Publishing}, + pages = {116023}, + file = {Chang et al_2017_Gyrokinetic projection of the divertor heat-flux width from present tokamaks to.pdf:/home/ym266336/Zotero/storage/JYXPL44I/Chang et al_2017_Gyrokinetic projection of the divertor heat-flux width from present tokamaks to.pdf:application/pdf}, +} + +@article{michels_full-f_2022, + title = {Full-f electromagnetic gyrokinetic turbulence simulations of the edge and scrape-off layer of {ASDEX} {Upgrade} with {GENE}-{X}}, + volume = {29}, + issn = {1070-664X}, + url = {https://doi.org/10.1063/5.0082413}, + doi = {10.1063/5.0082413}, + number = {3}, + urldate = {2022-10-04}, + journal = {Physics of Plasmas}, + author = {Michels, Dominik and Ulbl, Philipp and Zholobenko, Wladimir and Body, Thomas and Stegmeir, Andreas and Eich, Thomas and Griener, Michael and Conway, Garrard D. and Jenko, Frank}, + month = mar, + year = {2022}, + note = {Publisher: American Institute of Physics}, + pages = {032307}, + file = {Michels et al_2022_Full-f electromagnetic gyrokinetic turbulence simulations of the edge and.pdf:/home/ym266336/Zotero/storage/LMPWMVVE/Michels et al_2022_Full-f electromagnetic gyrokinetic turbulence simulations of the edge and.pdf:application/pdf}, +} diff --git a/simulations/geometryXVx/sheath/doc/sheath_equations.pdf b/simulations/geometryXVx/sheath/doc/sheath_equations.pdf new file mode 100644 index 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zVxeOe;353?n*g8ZuMm-uh4DXJEJQlRDKo8y>I1NU1s9TCwnGWCtC9TzqhC(0i{`5i z8*is%@(u+O0$G%aUXRc=ny%vu9fCAXxFj4+BpxRVK;ip6INUu?;V`YtrS=$S%g2vN z8Np;n%d{|#;A?(0n{2z?3dvv<0w@bg^UUz~>3UXRF{? zJ3mO-X!T~+ZoY%!r=H>CX8Hnwy@~G7!41X7xDtR41swTAcFxM`o0F=)Ys33;I_UHX zaHNAk{DXj}2}rqvpm#1H-!2gKFGTZ6t?aicL!xI564Hxiqle^NZ$gID7LJO=i*=dH zF6$S~1eq`T%@iF8t#2fmUuG$@AGf=X8qJEiwgcSU^qC8^cRG&p-GW+`w~t<4jhVCC zMnvvdtM?-VbRu{C4Dt^KbU4;}anD)tQgb8AvkaaJw*|%kVz|wPk*)FD_75@Ey5P!0 zkglrV92aEQlMI}(6~5VkY#{OdVo@1SSr-~x=mVHg;JaWgXvDXEZ*FwFl2K|L_? literal 0 HcmV?d00001 diff --git a/simulations/geometryXVx/sheath/doc/sheath_equations.tex b/simulations/geometryXVx/sheath/doc/sheath_equations.tex new file mode 100644 index 000000000..016adc878 --- /dev/null +++ b/simulations/geometryXVx/sheath/doc/sheath_equations.tex @@ -0,0 +1,87 @@ +\documentclass[11pt]{article} + +\usepackage[utf8]{inputenc} +\usepackage[T1]{fontenc} +\usepackage[english]{babel} +\usepackage{amsmath, amssymb} +\usepackage{biblatex} +\usepackage{csquotes} +\usepackage{graphics} +\usepackage{epsfig} +\usepackage{changepage} +\usepackage{amsmath} +\usepackage{amssymb} +\usepackage{amscd} +\usepackage{hyperref} +\usepackage{cleveref} +\addbibresource{library.bib} +\usepackage[margin=1.2in]{geometry} + + +\newcommand{\HRule}[1]{\rule{0.5\linewidth}{#1}} + +\begin{document} + +\begin{center} + \LARGE \textbf{Sheath equations} \\ + \vspace{0.8cm} +\end{center} + + +\section{Equations describing plasma-wall interaction} +\paragraph{Boltzmann-Poisson system} The \texttt{sheath} executable solves the following Boltzmann-Poisson system +% +\begin{eqnarray}\label{eq:boltzmann_eq_ref} + \partial_{t} f_a + v \partial_{x} f_a + \dfrac{q_a E}{m_a} \partial_{v} f_a = \mathcal{C}(f_a) + \mathcal{S}(f_a), \\[0.2cm] + -\partial_{x}^2 \phi = \rho / \varepsilon_0 \quad \text{with} \quad \rho = \sum\limits_{\mathrm{species}}^{} q_a n_a. +\end{eqnarray} +% +Where we use the $x$ variable to specify the position. The $v$ variable expresses the velocity of the considered particle. $f_a(v,x,t)$ is the distribution function of species $a$, which expresses the density of particles at time $t$ and at point $(x,v)$ of phase space. The subscript $a$ denotes the species the quantity refers to:---$\mathrm{e}$ for electrons, $\mathrm{i}$ for ions. The mass of any particle of species $a$ is written $m_a$, and its charge is $q_a$. $\varepsilon_0$ is the dielectric permittivity of vacuum. The electric field is written $E$, and we have $E = -\partial_{x} \phi$. We also introduced the local density $n_a$ of species $a$, which is a function of time and space. It is defined as the integral over the velocity space $n_a = \int_{}^{} dv \, f_a$. The $\mathcal{C}(f_a)$ term accounts for collisions, and the $\mathcal{S}(f_a)$ operator represents sources and sinks. Depending on the simulation parameters, these operators can be a combination of the terms described in the following. For more detail about each operator, see the corresponding documentation. \\ + +\noindent The Boltzmann-Poisson system is normalized using a reference density $n_0$ and temperature $T_0$. Time is normalized to the inverse of the electron plasma frequency $\omega_{\mathrm{pe_0}} = \sqrt{n_0 e^2 / m_\mathrm{e}\varepsilon_0} $. The space variable $x$ is normalized to the length scale relevant for plasma-wall interaction studies, i.e.\ the Debye length $\lambda_{\mathrm{D}_0} = \sqrt{\varepsilon_0 T_0 / n_0 e^2} $. The electrostatic potential is normalized to $T_0 / e$. The phase space velocity variable $v$ is normalized to the thermal velocity of each species $v_{T_0a}$ as $v_a = v/v_{T_0 a}$, with the thermal velocity of species $a$ written as $v_{T_0a} = \sqrt{T_0/m_a}$. Particles distribution functions are normalized to the reference particle density in phase space $n_0 / v_{T_0a}$. We use the notation $A_a = m_\mathrm{e} / m_a$ to express the mass ratio between electrons and species $a$ (in particular $A_\mathrm{e} = 1$). The normalized charge of species $a$ is written as $Z_a = q_a / e$. The normalized Boltzmann-Poisson system then reads as follows +% +\begin{eqnarray} + && \partial_{t} f_a + \sqrt{A_a} \left( v_a \partial_{x} f_a \right. - \left. Z_a \partial_{x} \phi \, \partial_{v_a} f_a \right) = \mathcal{C}(f_a) + \mathcal{S}(f_a), \label{eq:boltzmann_norm} \\[0.2cm] + && -\partial_{x}^2 \phi = \rho \quad \text{with} \quad \rho = \sum\limits_{\mathrm{species}}^{} Z_a n_a. \label{eq:poisson_norm} +\end{eqnarray} +% +In all the following each quantity of interest is normalized. If a reference to some dimensional quantities is needed, it will be explicitly pointed out. +% +\paragraph{Sources and sinks} The source term $\mathcal{S}(f_a)$ can be composed of the following operators. + +\begin{enumerate} + \item A Bhatnagar-Gross-Krook operator \cite{Bhatnagar1954} of the form + % + \begin{equation}\label{eq:bgk} + \mathcal{S}(f_a) = - \nu_{a}\mathcal{M}(x) \left( f_a - g \right), + \end{equation} + % +that relaxes the distribution function $f_a$ towards a target function $g$. Depending on the characteristics of the target function this operator can inject or absorb particles. The $\mathcal{M}(x)$ term is a function of space that defines the simulation region where the operator becomes active. Typically this function has a hyperbolic tangent shape and transitions smoothly between a region where it is equal to zero---therefore where the BGK operator is not active---and another region where it is equal to one. $\nu_{a}$ is a coefficient that sets the operator magnitude. This coefficient can be either a constant, or can be adapted at each spatial position and each timestep to ensure that this BGK term conserves the charge locally. +% +\item A source term \cite[Appendix A]{Sarazin2011} defined by +% +\begin{equation}\label{eq:general_form} + S(f_a) = s_\mathrm{k} \dfrac{\mathcal{M}(x)}{\int_{0}^{L_x} \mathcal{M}(x) \, dx} S_\mathrm{v}(v), +\end{equation} +% +where the mask function $\mathcal{M}$ defines the spatial extent of the source, similarly to its counterpart of Eq.~\ref{eq:bgk}. $L_x$ stands for the simulation box length. The $S_\mathrm{v}$ term is written as +% +\begin{equation}\label{eq:sv_expression} + S_\mathrm{v}(v) = \left\{ s_0\left( \dfrac{3}{2} - \dfrac{v^2}{2 T_\mathrm{s}} \right) + s_2 \left( -\dfrac{1}{2} + \dfrac{v^2}{2 T_\mathrm{s}} \right) \right\} \, \dfrac{1}{\sqrt{2 \pi T_\mathrm{s}} } \, e^{- \dfrac{v^2}{2 T_\mathrm{s}}} +\end{equation} +% + The $T_\mathrm{s}$ is a constant parameter that defines the source temperature. The $s_0$, $s_2$ and $s_\mathrm{k}$ parameters are numerical inputs of the code that define the properties of the source. In particular when using $s_0 = s_2 = 1$, the source adopts a Maxwellian shape whose magnitude is defined by the $s_\mathrm{k}$ parameter: +% +% +\begin{equation} + S(f_a) = s_\mathrm{k} \dfrac{\mathcal{M}(x)}{\int_{0}^{L_x} \mathcal{M}(x) \, dx}\dfrac{1}{\sqrt{2\pi T_\mathrm{s}}} \, e^{- \dfrac{v^2}{2 T_\mathrm{s}}}. +\end{equation} +% +\end{enumerate} +% +\paragraph{Collisions} The collisions term $\mathcal{C}(f_a)$ accounts for both intra and inter species collisions. \\ + +\noindent An extensive description of the source, sink and collision operators described above can be found in the \texttt{src/geometryXVx/rhs/doc} folder. + \clearpage + \printbibliography +\end{document} diff --git a/simulations/geometryXVx/sheath/pdi_out.yml.hpp b/simulations/geometryXVx/sheath/pdi_out.yml.hpp new file mode 100644 index 000000000..d96e2925d --- /dev/null +++ b/simulations/geometryXVx/sheath/pdi_out.yml.hpp @@ -0,0 +1,195 @@ +// SPDX-License-Identifier: MIT +#pragma once + +constexpr char const* const PDI_CFG = R"PDI_CFG( +metadata: + Nx_spline_cells : int + Nvx_spline_cells : int + iter : int + iter_start : int + time_saved : double + nbstep_diag: int + iter_saved : int + Lx : double + grid_x_extents: { type: array, subtype: int64, size: 1 } + grid_x: + type: array + subtype: double + size: [ '$grid_x_extents[0]' ] + grid_vx_extents: { type: array, subtype: int64, size: 1 } + grid_vx: + type: array + subtype: double + size: [ '$grid_vx_extents[0]' ] + MeshX_extents: { type: array, subtype: int64, size: 1 } + MeshX: + type: array + subtype: double + size: [ '$MeshX_extents[0]' ] + MeshVx_extents: { type: array, subtype: int64, size: 1 } + MeshVx: + type: array + subtype: double + size: [ '$MeshVx_extents[0]' ] + Nkinspecies: int + fdistribu_charges_extents : { type: array, subtype: int64, size: 1 } + fdistribu_charges: + type: array + subtype: double + size: [ '$fdistribu_charges_extents[0]' ] + fdistribu_masses_extents : { type: array, subtype: int64, size: 1 } + fdistribu_masses: + type: array + subtype: double + size: [ '$fdistribu_masses_extents[0]' ] + fdistribu_eq_extents : { type: array, subtype: int64, size: 2 } + fdistribu_eq: + type: array + subtype: double + size: [ '$fdistribu_eq_extents[0]', '$fdistribu_eq_extents[1]' ] + collintra_nustar0 : double + collinter_nustar0 : double + + krook_sink_adaptive_extent : double + krook_sink_adaptive_stiffness : double + krook_sink_adaptive_amplitude : double + krook_sink_adaptive_density : double + krook_sink_adaptive_temperature : double + krook_sink_adaptive_mask_extents: { type: array, subtype: int64, size: 1 } + krook_sink_adaptive_mask: + type: array + subtype: double + size: [ '$krook_sink_adaptive_mask_extents[0]' ] + krook_sink_adaptive_ftarget_extents: { type: array, subtype: int64, size: 1 } + krook_sink_adaptive_ftarget: + type: array + subtype: double + size: [ '$krook_sink_adaptive_ftarget_extents[0]' ] + + krook_sink_constant_extent : double + krook_sink_constant_stiffness : double + krook_sink_constant_amplitude : double + krook_sink_constant_density : double + krook_sink_constant_temperature : double + krook_sink_constant_mask_extents: { type: array, subtype: int64, size: 1 } + krook_sink_constant_mask: + type: array + subtype: double + size: [ '$krook_sink_constant_mask_extents[0]' ] + krook_sink_constant_ftarget_extents: { type: array, subtype: int64, size: 1 } + krook_sink_constant_ftarget: + type: array + subtype: double + size: [ '$krook_sink_constant_ftarget_extents[0]' ] + + kinetic_source_extent : double + kinetic_source_stiffness : double + kinetic_source_amplitude : double + kinetic_source_density : double + kinetic_source_energy : double + kinetic_source_temperature : double + kinetic_source_velocity_shape_extents: { type: array, subtype: int64, size: 1 } + kinetic_source_velocity_shape: + type: array + subtype: double + size: [ '$kinetic_source_velocity_shape_extents[0]' ] + kinetic_source_spatial_extent_extents: { type: array, subtype: int64, size: 1 } + kinetic_source_spatial_extent: + type: array + subtype: double + size: [ '$kinetic_source_spatial_extent_extents[0]' ] + + filename_size: size_t + filename: {type: array, subtype: char, size: "$filename_size"} + +data: + fdistribu_extents: { type: array, subtype: int64, size: 3 } + fdistribu: + type: array + subtype: double + size: [ '$fdistribu_extents[0]', '$fdistribu_extents[1]', '$fdistribu_extents[2]' ] + electrostatic_potential_extents: { type: array, subtype: int64, size: 1 } + electrostatic_potential: + type: array + subtype: double + size: [ '$electrostatic_potential_extents[0]' ] + +plugins: + set_value: + on_init: + - share: + - iter_saved: 0 + on_data: + iter: + - set: + - iter_saved: '${iter_start} + ${iter}/${nbstep_diag}' + on_finalize: + - release: [iter_saved] + decl_hdf5: + - file: 'VOICEXX_initstate.h5' + on_event: [initial_state] + collision_policy: replace_and_warn + write: + - Nx_spline_cells + - Nvx_spline_cells + - MeshX + - MeshVx + - Lx + - nbstep_diag + - collintra_nustar0 + - collinter_nustar0 + - Nkinspecies + - fdistribu_charges + - fdistribu_masses + - fdistribu_eq + + - krook_sink_adaptive_extent + - krook_sink_adaptive_stiffness + - krook_sink_adaptive_amplitude + - krook_sink_adaptive_density + - krook_sink_adaptive_temperature + - krook_sink_adaptive_mask + - krook_sink_adaptive_ftarget + + - krook_sink_constant_extent + - krook_sink_constant_stiffness + - krook_sink_constant_amplitude + - krook_sink_constant_density + - krook_sink_constant_temperature + - krook_sink_constant_mask + - krook_sink_constant_ftarget + + - kinetic_source_extent + - kinetic_source_stiffness + - kinetic_source_amplitude + - kinetic_source_density + - kinetic_source_energy + - kinetic_source_temperature + - kinetic_source_velocity_shape + - kinetic_source_spatial_extent + - file: 'VOICEXX_${iter_saved:05}.h5' + on_event: [iteration, last_iteration] + when: '${iter} % ${nbstep_diag} = 0' + collision_policy: replace_and_warn + write: [time_saved, fdistribu, electrostatic_potential] + - file: 'VOICEXX_${iter_start:05}.h5' + on_event: restart + read: [time_saved, fdistribu] + - file: '${filename}' + on_event: [read_x_extents] + read: + grid_x_extents: {size_of: grid_x} + - file: '${filename}' + on_event: [read_x] + read: + grid_x: ~ + - file: '${filename}' + on_event: [read_vx_extents] + read: + grid_vx_extents: {size_of: grid_vx} + - file: '${filename}' + on_event: [read_vx] + read: + grid_vx: ~ + #trace: ~ +)PDI_CFG"; diff --git a/simulations/geometryXVx/sheath/ref_simulation/figures/charge_density_t990.0.png b/simulations/geometryXVx/sheath/ref_simulation/figures/charge_density_t990.0.png new file mode 100644 index 0000000000000000000000000000000000000000..e3986253ca0f80fcd90593bdf3e2e1581b54ce52 GIT binary patch literal 67916 zcmeFZc{r6@_&>Z$rASJl$WTZKl_YZ-u*p2nNtw1GnYRp)B%u__oFVg+d2TSA$~@1C zG7pJuXV|>=QtJD?-uJKf-{0?C=Um6dv!DH}weEG__h(p-zp|nX6$JwY27{r(%3e{$ 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z`RWqb3=T!exoV+BMHgEqC#(qr1;fSKhK8Z&_Ans-g?5Z!Zlq3q$k}Vvq}m^%WhiV5 z2Zh3UdNr9l5c$PpMvsaVjnTk4lZxd_Ekafo**EblCrk@+11j<~H*_31%`snwZDprW zOx{Xb6Z6Cd-xs`Z`1)J +#include +#include +#include +#include +#include +#include +#include +#include +#include + +#include +#include + +#include +#include + +#include "bsl_advection_vx.hpp" +#include "bsl_advection_x.hpp" +#include "chargedensitycalculator.hpp" +#include "collisions_inter.hpp" +#include "collisions_intra.hpp" +#include "ddc_alias_inline_functions.hpp" +#include "fem_1d_poisson_solver.hpp" +#include "fft_poisson_solver.hpp" +#include "geometry.hpp" +#include "input.hpp" +#include "irighthandside.hpp" +#include "kinetic_source.hpp" +#include "krook_source_adaptive.hpp" +#include "krook_source_constant.hpp" +#include "maxwellianequilibrium.hpp" +#include "neumann_spline_quadrature.hpp" +#include "output.hpp" +#include "paraconfpp.hpp" +#include "pdi_out.yml.hpp" +#include "predcorr.hpp" +#include "qnsolver.hpp" +#include "restartinitialization.hpp" +#include "sheath.yaml.hpp" +#include "singlemodeperturbinitialization.hpp" +#include "species_info.hpp" +#include "species_init.hpp" +#include "spline_interpolator.hpp" +#include "splitrighthandsidesolver.hpp" +#include "splitvlasovsolver.hpp" + +using std::cerr; +using std::endl; +using std::chrono::steady_clock; +namespace fs = std::filesystem; + +int main(int argc, char** argv) +{ + // Environments variables for profiling + setenv("KOKKOS_TOOLS_LIBS", KP_KERNEL_TIMER_PATH, false); + setenv("KOKKOS_TOOLS_TIMER_JSON", "true", false); + + long int iter_start; + PC_tree_t conf_voicexx; + parse_executable_arguments( + conf_voicexx, + iter_start, + argc, + argv, + (std::string(mesh_params_yaml) + std::string(params_yaml)).c_str()); + PC_tree_t conf_pdi = PC_parse_string(PDI_CFG); + PC_errhandler(PC_NULL_HANDLER); + PDI_init(conf_pdi); + + Kokkos::ScopeGuard kokkos_scope(argc, argv); + ddc::ScopeGuard ddc_scope(argc, argv); + +#ifdef INPUT_MESH + std::string spline_mesh_filename(PCpp_string(conf_voicexx, ".SplineMesh.grid_file")); + size_t spline_mesh_filename_size = spline_mesh_filename.size(); + PDI_multi_expose( + "setFilename", + "filename_size", + &spline_mesh_filename_size, + PDI_OUT, + "filename", + spline_mesh_filename.c_str(), + PDI_OUT, + NULL); +#endif + + // Reading config + // --> Mesh info + IdxRangeX const mesh_x = init_spline_dependent_idx_range< + GridX, + BSplinesX, + SplineInterpPointsX>(conf_voicexx, "x"); + IdxRangeVx const mesh_vx = init_spline_dependent_idx_range< + GridVx, + BSplinesVx, + SplineInterpPointsVx>(conf_voicexx, "vx"); + IdxRangeXVx const meshXVx(mesh_x, mesh_vx); + + IdxRangeSp const idx_range_kinsp = init_species(conf_voicexx); + + IdxRangeSpXVx const meshSpXVx(idx_range_kinsp, meshXVx); + IdxRangeSpVx const meshSpVx(idx_range_kinsp, mesh_vx); + + SplineXBuilder const builder_x(meshXVx); +#if !defined(PERIODIC_RDIMX) || defined(INPUT_MESH) + SplineXBuilder_1d const builder_x_poisson(mesh_x); +#endif + SplineVxBuilder const builder_vx(meshXVx); + + // Initialization of the distribution function + DFieldMemSpVx allfequilibrium(meshSpVx); + MaxwellianEquilibrium const init_fequilibrium + = MaxwellianEquilibrium::init_from_input(idx_range_kinsp, conf_voicexx); + init_fequilibrium(allfequilibrium); + + ddc::expose_to_pdi("iter_start", iter_start); + + DFieldMemSpXVx allfdistribu(meshSpXVx); + double time_start(0); + if (iter_start == 0) { + SingleModePerturbInitialization const init = SingleModePerturbInitialization:: + init_from_input(allfequilibrium, idx_range_kinsp, conf_voicexx); + init(allfdistribu); + } else { + RestartInitialization const restart(iter_start, time_start); + restart(allfdistribu); + } + auto allfequilibrium_host = ddc::create_mirror_view_and_copy(get_field(allfequilibrium)); + + // --> Algorithm info + double const deltat = PCpp_double(conf_voicexx, ".Algorithm.deltat"); + int const nbiter = static_cast(PCpp_int(conf_voicexx, ".Algorithm.nbiter")); + + // --> Output info + double const time_diag = PCpp_double(conf_voicexx, ".Output.time_diag"); + int const nbstep_diag = int(time_diag / deltat); + +#ifdef PERIODIC_RDIMX + ddc::PeriodicExtrapolationRule bv_x_min; + ddc::PeriodicExtrapolationRule bv_x_max; +#else + ddc::ConstantExtrapolationRule bv_x_min(ddc::coordinate(mesh_x.front())); + ddc::ConstantExtrapolationRule bv_x_max(ddc::coordinate(mesh_x.back())); +#endif + + ddc::ConstantExtrapolationRule bv_vx_min(ddc::coordinate(mesh_vx.front())); + ddc::ConstantExtrapolationRule bv_vx_max(ddc::coordinate(mesh_vx.back())); + + // Creating operators + SplineXEvaluator const spline_x_evaluator(bv_x_min, bv_x_max); + SplineVxEvaluator const spline_vx_evaluator(bv_vx_min, bv_vx_max); +#if !defined(PERIODIC_RDIMX) || defined(INPUT_MESH) + SplineXEvaluator_1d const spline_x_evaluator_poisson(bv_x_min, bv_x_max); +#endif + PreallocatableSplineInterpolator const spline_x_interpolator(builder_x, spline_x_evaluator); + PreallocatableSplineInterpolator const spline_vx_interpolator(builder_vx, spline_vx_evaluator); + + BslAdvectionSpatial const advection_x(spline_x_interpolator); + BslAdvectionVelocity const advection_vx(spline_vx_interpolator); + + // list of rhs operators + std::vector> rhs_operators; + std::vector krook_source_constant_vector; + std::vector krook_source_adaptive_vector; + // Krook operators initialization + int const nb_rhsKrook(PCpp_len(conf_voicexx, ".Krook")); + for (int ik = 0; ik < nb_rhsKrook; ++ik) { + // --> Krook info + PC_tree_t const conf_krook = PCpp_get(conf_voicexx, ".Krook[%d]", ik); + + static std::map + str2rhstype {{"source", RhsType::Source}, {"sink", RhsType::Sink}}; + RhsType type = str2rhstype[PCpp_string(conf_krook, ".type")]; + std::string const krook_name = PCpp_string(conf_krook, ".name"); + if (krook_name == "constant") { + krook_source_constant_vector.emplace_back( + mesh_x, + mesh_vx, + type, + PCpp_double(conf_krook, ".extent"), + PCpp_double(conf_krook, ".stiffness"), + PCpp_double(conf_krook, ".amplitude"), + PCpp_double(conf_krook, ".density"), + PCpp_double(conf_krook, ".temperature")); + rhs_operators.emplace_back(krook_source_constant_vector.back()); + + } else if (krook_name == "adaptive") { + krook_source_adaptive_vector.emplace_back( + mesh_x, + mesh_vx, + type, + PCpp_double(conf_krook, ".extent"), + PCpp_double(conf_krook, ".stiffness"), + PCpp_double(conf_krook, ".amplitude"), + PCpp_double(conf_krook, ".density"), + PCpp_double(conf_krook, ".temperature")); + rhs_operators.emplace_back(krook_source_adaptive_vector.back()); + } else { + throw std::invalid_argument( + "Invalid krook name, allowed values are: 'constant', or 'adaptive'."); + } + } + + // Kinetic source + KineticSource const rhs_kinetic_source( + mesh_x, + mesh_vx, + PCpp_double(conf_voicexx, ".KineticSource.extent"), + PCpp_double(conf_voicexx, ".KineticSource.stiffness"), + PCpp_double(conf_voicexx, ".KineticSource.amplitude"), + PCpp_double(conf_voicexx, ".KineticSource.density"), + PCpp_double(conf_voicexx, ".KineticSource.energy"), + PCpp_double(conf_voicexx, ".KineticSource.temperature")); + rhs_operators.emplace_back(rhs_kinetic_source); + + + CollisionsIntra const + collisions_intra(meshSpXVx, PCpp_double(conf_voicexx, ".CollisionsInfo.nustar0")); + rhs_operators.emplace_back(collisions_intra); + + std::optional collisions_inter; + if (PCpp_bool(conf_voicexx, ".CollisionsInfo.enable_inter")) { + collisions_inter.emplace(meshSpXVx, PCpp_double(conf_voicexx, ".CollisionsInfo.nustar0")); + rhs_operators.emplace_back(*collisions_inter); + } + SplitVlasovSolver const vlasov(advection_x, advection_vx); + SplitRightHandSideSolver const boltzmann(vlasov, rhs_operators); + + DFieldMemVx const quadrature_coeffs(neumann_spline_quadrature_coefficients< + Kokkos::DefaultExecutionSpace>(mesh_vx, builder_vx)); + + ChargeDensityCalculator rhs(get_const_field(quadrature_coeffs)); +#if defined(PERIODIC_RDIMX) && !defined(INPUT_MESH) + FFTPoissonSolver poisson_solver(mesh_x); +#else + FEM1DPoissonSolver poisson_solver(builder_x_poisson, spline_x_evaluator_poisson); +#endif + QNSolver const poisson(poisson_solver, rhs); + + PredCorr const predcorr(boltzmann, poisson); + + // Starting the code + ddc::expose_to_pdi("Nx_spline_cells", ddc::discrete_space().ncells()); + ddc::expose_to_pdi("Nvx_spline_cells", ddc::discrete_space().ncells()); + expose_mesh_to_pdi("MeshX", mesh_x); + expose_mesh_to_pdi("MeshVx", mesh_vx); + ddc::expose_to_pdi("Lx", ddcHelper::total_interval_length(mesh_x)); + ddc::expose_to_pdi("nbstep_diag", nbstep_diag); + ddc::expose_to_pdi("Nkinspecies", idx_range_kinsp.size()); + ddc::expose_to_pdi( + "fdistribu_charges", + ddc::discrete_space().charges()[idx_range_kinsp]); + ddc::expose_to_pdi( + "fdistribu_masses", + ddc::discrete_space().masses()[idx_range_kinsp]); + ddc::PdiEvent("initial_state").with("fdistribu_eq", allfequilibrium_host); + + steady_clock::time_point const start = steady_clock::now(); + + predcorr(allfdistribu, time_start, deltat, nbiter); + + steady_clock::time_point const end = steady_clock::now(); + + double const simulation_time = std::chrono::duration(end - start).count(); + std::cout << "Simulation time: " << simulation_time << "s\n"; + + PC_tree_destroy(&conf_pdi); + + PDI_finalize(); + + PC_tree_destroy(&conf_voicexx); + + return EXIT_SUCCESS; +} diff --git a/simulations/geometryXVx/sheath/sheath.yaml.hpp b/simulations/geometryXVx/sheath/sheath.yaml.hpp new file mode 100644 index 000000000..8295f607b --- /dev/null +++ b/simulations/geometryXVx/sheath/sheath.yaml.hpp @@ -0,0 +1,73 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#ifdef INPUT_MESH +constexpr char const* const mesh_params_yaml = R"PARAMS_CFG(SplineMesh: + x_min: 0.0 + x_max: 50 + x_ncells: 512 + vx_min: -6.0 + vx_max: +6.0 + vx_ncells: 256 + grid_file: "grids.h5" + +)PARAMS_CFG"; +#else +constexpr char const* const mesh_params_yaml = R"PARAMS_CFG(SplineMesh: + x_min: 0.0 + x_max: 50 + x_ncells: 512 + vx_min: -6.0 + vx_max: +6.0 + vx_ncells: 256 + +)PARAMS_CFG"; +#endif + +constexpr char const* const params_yaml = R"PARAMS_CFG(SpeciesInfo: +- charge: -1. + mass: 1. + density_eq: 1. + temperature_eq: 1. + mean_velocity_eq: 0. + perturb_amplitude: 0. + perturb_mode: 1 + +- charge: 1. + mass: 400. + density_eq: 1. + temperature_eq: 1. + mean_velocity_eq: 0. + perturb_amplitude: 0. + perturb_mode: 1 + +Krook: + - name: 'adaptive' # 'constant' or adaptive': constant values or not for nu coeff. + type: 'sink' + solver: 'rk2' # possible values : 'rk2' + extent: 0.20 + stiffness: 1 + amplitude: 0.1 + density: 1e-9 + temperature: 0.5 + +KineticSource: + extent: 0.45 + stiffness: 4 + amplitude: 0.1 + density: 1. + energy: 1. + temperature: 1. + +CollisionsInfo: + enable_inter: true + nustar0: 0.1 + +Algorithm: + deltat: 0.1 + nbiter: 50 + +Output: + time_diag: 0.1 +)PARAMS_CFG"; diff --git a/src/geometryXVx/CMakeLists.txt b/src/geometryXVx/CMakeLists.txt index ea79cf17d..beea381bd 100644 --- a/src/geometryXVx/CMakeLists.txt +++ b/src/geometryXVx/CMakeLists.txt @@ -3,7 +3,9 @@ add_subdirectory(poisson) add_subdirectory(geometry) +add_subdirectory(geometryMX) add_subdirectory(time_integration) +add_subdirectory(time_integration_hybrid) add_subdirectory(rhs) add_subdirectory(boltzmann) add_subdirectory(initialization) diff --git a/src/geometryXVx/README.md b/src/geometryXVx/README.md index a62629e88..593ae916b 100644 --- a/src/geometryXVx/README.md +++ b/src/geometryXVx/README.md @@ -4,8 +4,10 @@ The `geometryXVx` folder contains all the code describing methods which are spec - [boltzmann](./boltzmann/README.md) : Solvers for a Boltzmann equation. - [geometry](./geometry/README.md) : All the dimension tags used for a simulation in the geometry. +- [geometryMX](./geometryMX/README.md) : Code describing a geometry with a single spatial dimension and a single fluid moment dimension. - [initialization](./initialization/README.md) : Initialization methods for the distribution function. - [poisson](./poisson/README.md) : Code describing the Quasi-Neutrality solver. - [rhs](./rhs/README.md) : Code describing the operators on the right hand side of the Boltzmann equation; namely sources, sinks and collisions. - [time\_integration](./time_integration/README.md) : Time integrators for a Boltzmann-Poisson system of equations. +- [time\_integration\_hybrid](./time_integration_hybrid/README.md) : Time integrators for a Boltzmann-Poisson system of equations, with a fluid neutral species. - [utils](./utils/README.md) : Miscellaneous utility functions. diff --git a/src/geometryXVx/geometry/geometry.hpp b/src/geometryXVx/geometry/geometry.hpp index dc5b935ad..a2b7adf3b 100644 --- a/src/geometryXVx/geometry/geometry.hpp +++ b/src/geometryXVx/geometry/geometry.hpp @@ -60,13 +60,8 @@ using CoordXVx = Coord; int constexpr BSDegreeX = 3; int constexpr BSDegreeVx = 3; -#ifdef INPUT_MESH -bool constexpr BsplineOnUniformCellsX = false; -bool constexpr BsplineOnUniformCellsVx = false; -#else bool constexpr BsplineOnUniformCellsX = true; bool constexpr BsplineOnUniformCellsVx = true; -#endif struct BSplinesX : std::conditional_t< diff --git a/src/geometryXVx/geometryMX/CMakeLists.txt b/src/geometryXVx/geometryMX/CMakeLists.txt new file mode 100644 index 000000000..08c824db1 --- /dev/null +++ b/src/geometryXVx/geometryMX/CMakeLists.txt @@ -0,0 +1,6 @@ +# SPDX-License-Identifier: MIT + +add_subdirectory(fluidinitialization) +add_subdirectory(fluidtransportsolver) +add_subdirectory(reactionrates) +add_subdirectory(kineticfluidcoupling) \ No newline at end of file diff --git a/src/geometryXVx/geometryMX/README.md b/src/geometryXVx/geometryMX/README.md new file mode 100644 index 000000000..fbe065438 --- /dev/null +++ b/src/geometryXVx/geometryMX/README.md @@ -0,0 +1,8 @@ +# Geometry (x) + +The `geometryMX` folder contains all the code describing methods which are specific to a geometry with 1 spatial dimension and one dimension describing fluid moments (ex: density, temperature, mean velocity). It is broken up into the following sub-folders: + +- [fluidinitialization](./fluidinitialization/README.md) : Initialization methods for fluid species. +- [fluidtransportsolver](./fluidtransportsolver/README.md) : Solver for fluid models transport. +- [kineticfluidcoupling](./kineticfluidcoupling/README.md) : Solver for sources in fluid and kinetic equations. +- [reactionrates](./reactionrates/README.md) : Reaction rate calculations. \ No newline at end of file diff --git a/src/geometryXVx/geometryMX/fluidinitialization/CMakeLists.txt b/src/geometryXVx/geometryMX/fluidinitialization/CMakeLists.txt new file mode 100644 index 000000000..ccbc986a1 --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidinitialization/CMakeLists.txt @@ -0,0 +1,23 @@ +# SPDX-License-Identifier: MIT + +foreach(GEOMETRY_VARIANT IN LISTS GEOMETRY_XVx_VARIANTS_LIST) + +add_library("fluidinitialization_${GEOMETRY_VARIANT}" STATIC + constantfluidinitialization.cpp +) + +target_include_directories("fluidinitialization_${GEOMETRY_VARIANT}" + PUBLIC "${CMAKE_CURRENT_SOURCE_DIR}" +) + +target_link_libraries("fluidinitialization_${GEOMETRY_VARIANT}" + PUBLIC + DDC::DDC + gslx::geometry_${GEOMETRY_VARIANT} + gslx::utils + +) + +add_library("gslx::fluidinitialization_${GEOMETRY_VARIANT}" ALIAS "fluidinitialization_${GEOMETRY_VARIANT}") + +endforeach() diff --git a/src/geometryXVx/geometryMX/fluidinitialization/README.md b/src/geometryXVx/geometryMX/fluidinitialization/README.md new file mode 100644 index 000000000..63448e17e --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidinitialization/README.md @@ -0,0 +1,6 @@ +# Fluid Initialization methods + +The fluidinitialization folder contains any methods that define the value of a fluid species at the start of the simulation. The fluid species is described by its fluid moments. + +The implemented initialization methods are: +- ConstantFluidInitialization \ No newline at end of file diff --git a/src/geometryXVx/geometryMX/fluidinitialization/constantfluidinitialization.cpp b/src/geometryXVx/geometryMX/fluidinitialization/constantfluidinitialization.cpp new file mode 100644 index 000000000..dd4feccae --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidinitialization/constantfluidinitialization.cpp @@ -0,0 +1,24 @@ +// SPDX-License-Identifier: MIT + +#include + +#include "constantfluidinitialization.hpp" + +ConstantFluidInitialization::ConstantFluidInitialization(host_t moments) + : m_moments_alloc(get_idx_range(moments)) +{ + ddc::parallel_deepcopy(m_moments_alloc, moments); +} + +DFieldSpMomX ConstantFluidInitialization::operator()(DFieldSpMomX const fluid_moments) const +{ + DConstFieldSpMom moments(get_field(m_moments_alloc)); + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + get_idx_range(fluid_moments), + KOKKOS_LAMBDA(IdxSpMomX const ispmx) { + IdxSpMom ispm(ddc::select(ispmx)); + fluid_moments(ispmx) = moments(ispm); + }); + return fluid_moments; +} diff --git a/src/geometryXVx/geometryMX/fluidinitialization/constantfluidinitialization.hpp b/src/geometryXVx/geometryMX/fluidinitialization/constantfluidinitialization.hpp new file mode 100644 index 000000000..4ab94e2aa --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidinitialization/constantfluidinitialization.hpp @@ -0,0 +1,30 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#include "geometry.hpp" +#include "ifluidinitialization.hpp" +/** + * @brief A class that initializes a fluid species with constant moments. + */ +class ConstantFluidInitialization : public IFluidInitialization +{ + DFieldMemSpMom m_moments_alloc; + +public: + /** + * @brief Creates an instance of the ConstantFluidInitialization class. + * @param[in] moments The fluid moments the fluid species should be initialized with. + */ + ConstantFluidInitialization(host_t moments); + + ~ConstantFluidInitialization() override = default; + + /** + * @brief Initializes the fluid species with a constant moments. + * @param[inout] fluid_moments On input: a field referencing an uninitialized fluid species described through its moments. + * On output: a field referencing a the fluid species initialized with constant moments. + * @return A field referencing the initialized fluid species. + */ + DFieldSpMomX operator()(DFieldSpMomX const fluid_moments) const override; +}; diff --git a/src/geometryXVx/geometryMX/fluidinitialization/ifluidinitialization.hpp b/src/geometryXVx/geometryMX/fluidinitialization/ifluidinitialization.hpp new file mode 100644 index 000000000..1b970c6cb --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidinitialization/ifluidinitialization.hpp @@ -0,0 +1,21 @@ +// SPDX-License-Identifier: MIT +#pragma once + +#include "geometry.hpp" + +/** + * @brief An abstract class that allows for initializing a fluid species. + */ +class IFluidInitialization +{ +public: + virtual ~IFluidInitialization() = default; + + /** + * @brief Operator for initializing a neutral species. + * @param[in, out] fluid_moments On input: the uninitialized fluid species. + * On output: the initialized fluid species. + * @return A field referencing the initialized fluid species. + */ + virtual DFieldSpMomX operator()(DFieldSpMomX fluid_moments) const = 0; +}; diff --git a/src/geometryXVx/geometryMX/fluidtransportsolver/CMakeLists.txt b/src/geometryXVx/geometryMX/fluidtransportsolver/CMakeLists.txt new file mode 100644 index 000000000..279562260 --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidtransportsolver/CMakeLists.txt @@ -0,0 +1,32 @@ +# SPDX-License-Identifier: MIT + +foreach(GEOMETRY_VARIANT IN LISTS GEOMETRY_XVx_VARIANTS_LIST) + +add_library("fluidsolver_${GEOMETRY_VARIANT}" STATIC + diffusiveneutralsolver.cpp + nullfluidsolver.cpp +) + +target_include_directories("fluidsolver_${GEOMETRY_VARIANT}" + PUBLIC "${CMAKE_CURRENT_SOURCE_DIR}" +) + +target_link_libraries("fluidsolver_${GEOMETRY_VARIANT}" + PUBLIC + DDC::DDC + sll::SLL + gslx::advection + gslx::geometry_${GEOMETRY_VARIANT} + gslx::interpolation + gslx::quadrature + gslx::speciesinfo + gslx::reactionrates_${GEOMETRY_VARIANT} + gslx::speciesinfo + gslx::timestepper + gslx::utils + +) + +add_library("gslx::fluidsolver_${GEOMETRY_VARIANT}" ALIAS "fluidsolver_${GEOMETRY_VARIANT}") + +endforeach() diff --git a/src/geometryXVx/geometryMX/fluidtransportsolver/README.md b/src/geometryXVx/geometryMX/fluidtransportsolver/README.md new file mode 100644 index 000000000..07ead767c --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidtransportsolver/README.md @@ -0,0 +1,7 @@ +# Fluid transport solvers (MX) + +The `fluidtransportsolver` folder contains code that allows solving for models that describe a species considered as fluid. Such a fluid species is described by moments of the distribution function (density, particle flux, energy...) rather than by a complete distribution function. Equations describing the time evolution of such a fluid moments are called *fluid equations*. Such fluid equations describe the conservation of fluid moments: conservation of density, particle flux, energy, etc. + +The currently implemented solvers are : +- DiffusiveNeutralSolver +- NullFluidSolver diff --git a/src/geometryXVx/geometryMX/fluidtransportsolver/diffusiveneutralsolver.cpp b/src/geometryXVx/geometryMX/fluidtransportsolver/diffusiveneutralsolver.cpp new file mode 100644 index 000000000..26c490a7a --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidtransportsolver/diffusiveneutralsolver.cpp @@ -0,0 +1,231 @@ +// SPDX-License-Identifier: MIT + +#include "diffusiveneutralsolver.hpp" +#include "quadrature.hpp" +#include "rk2.hpp" +#include "trapezoid_quadrature.hpp" + + +DiffusiveNeutralSolver::DiffusiveNeutralSolver( + IReactionRate const& charge_exchange, + IReactionRate const& ionization, + IReactionRate const& recombination, + double const normalization_coeff, + SplineXBuilder_1d const& spline_x_builder, + SplineXEvaluator_1d const& spline_x_evaluator, + DConstFieldVx const& quadrature_coeffs) + : m_charge_exchange(charge_exchange) + , m_ionization(ionization) + , m_recombination(recombination) + , m_normalization_coeff(normalization_coeff) + , m_spline_x_builder(spline_x_builder) + , m_spline_x_evaluator(spline_x_evaluator) + , m_quadrature_coeffs(quadrature_coeffs) +{ +} + +IdxSp DiffusiveNeutralSolver::find_ion(IdxRangeSp const idx_range_kinsp) const +{ + bool ion_found = false; + IdxSp iion; + for (IdxSp const isp : idx_range_kinsp) { + if (charge(isp) > 0.) { + ion_found = true; + iion = isp; + } + } + if (!ion_found) { + throw std::runtime_error("ion not found"); + } + assert(idx_range_kinsp.size() == 2); + + return iion; +} + +void DiffusiveNeutralSolver::get_derivative( + DFieldSpMomX dn, + DConstFieldSpMomX neutrals, + DConstFieldSpX density, + DConstFieldSpX velocity, + DConstFieldSpX temperature) const +{ + IdxRangeSpX idx_range_fluidspx(get_idx_range(neutrals)); + + // building reaction rates + DFieldMemSpX charge_exchange_rate_alloc(idx_range_fluidspx); + DFieldMemSpX ionization_rate_alloc(idx_range_fluidspx); + DFieldMemSpX recombination_rate_alloc(idx_range_fluidspx); + + DFieldSpX charge_exchange_rate = get_field(charge_exchange_rate_alloc); + DFieldSpX ionization_rate = get_field(ionization_rate_alloc); + DFieldSpX recombination_rate = get_field(recombination_rate_alloc); + + m_charge_exchange(charge_exchange_rate, density, temperature); + m_ionization(ionization_rate, density, temperature); + m_recombination(recombination_rate, density, temperature); + + // compute diffusive model equation terms + DFieldMemSpX density_equilibrium_velocity_alloc(idx_range_fluidspx); + DFieldMemSpX diffusion_temperature_alloc(idx_range_fluidspx); + DFieldSpX density_equilibrium_velocity = get_field(density_equilibrium_velocity_alloc); + DFieldSpX diffusion_temperature = get_field(diffusion_temperature_alloc); + + IdxSp const iion(find_ion(get_idx_range(density))); + IdxMom const ineutral_density(0); + + double const normalization_coeff_alpha0(m_normalization_coeff); + double const mass_ratio(mass(ielec()) / mass(iion)); + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + idx_range_fluidspx, + KOKKOS_LAMBDA(IdxSpX const ifspx) { + IdxSp const isp(ddc::select(ifspx)); + IdxX const ix(ddc::select(ifspx)); + + double const denom = density(iion, ix) * charge_exchange_rate(ifspx) + + density(ielec(), ix) * ionization_rate(ifspx); + + density_equilibrium_velocity(ifspx) + = (density(ielec(), ix) * density(iion, ix) * recombination_rate(ifspx) + + neutrals(ifspx, ineutral_density) * density(iion, ix) + * charge_exchange_rate(ifspx)) + * velocity(iion, ix) * Kokkos::sqrt(mass_ratio) / denom; + + diffusion_temperature(ifspx) + = normalization_coeff_alpha0 * temperature(iion, ix) / (mass(isp) * denom); + + // density source is not solved here, we only solve transport. + }); + + // compute coordinates at which spatial derivatives are evaluated + FieldMemX coords_eval_alloc(get_idx_range(neutrals)); + auto coords_eval = get_field(coords_eval_alloc); + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + get_idx_range(neutrals), + KOKKOS_LAMBDA(IdxX const ix) { coords_eval(ix) = ddc::coordinate(ix); }); + + // create chunks to store spatial derivatives + DFieldMemSpX gradx_density_equilibrium_velocity_alloc(idx_range_fluidspx); + DFieldMemSpX gradx_diffusion_temperature_alloc(idx_range_fluidspx); + DFieldMemSpX gradx_neutrals_density_alloc(idx_range_fluidspx); + DFieldMemSpX laplx_neutrals_density_alloc(idx_range_fluidspx); + + DFieldSpX gradx_density_equilibrium_velocity + = get_field(gradx_density_equilibrium_velocity_alloc); + DFieldSpX gradx_diffusion_temperature = get_field(gradx_diffusion_temperature_alloc); + DFieldSpX gradx_neutrals_density = get_field(gradx_neutrals_density_alloc); + DFieldSpX laplx_neutrals_density = get_field(laplx_neutrals_density_alloc); + + ddc::for_each(get_idx_range(neutrals), [&](IdxSp const isp) { + // compute spline coefficients + DBSFieldMemX density_equilibrium_velocity_spline_x_coeff( + get_spline_idx_range(m_spline_x_builder)); + + DBSFieldMemX diffusion_temperature_spline_x_coeff(get_spline_idx_range(m_spline_x_builder)); + + DBSFieldMemX neutrals_density_spline_x_coeff(get_spline_idx_range(m_spline_x_builder)); + + m_spline_x_builder( + get_field(density_equilibrium_velocity_spline_x_coeff), + get_const_field(density_equilibrium_velocity[isp])); + + m_spline_x_builder( + get_field(diffusion_temperature_spline_x_coeff), + get_const_field(diffusion_temperature[isp])); + + m_spline_x_builder( + get_field(neutrals_density_spline_x_coeff), + get_const_field(neutrals[IdxSpMom(isp, ineutral_density)])); + + // compute gradients + m_spline_x_evaluator + .deriv(get_field(gradx_density_equilibrium_velocity[isp]), + get_const_field(coords_eval), + get_const_field(density_equilibrium_velocity_spline_x_coeff)); + + m_spline_x_evaluator + .deriv(gradx_diffusion_temperature[isp], + get_const_field(coords_eval), + get_const_field(diffusion_temperature_spline_x_coeff)); + + m_spline_x_evaluator + .deriv(gradx_neutrals_density[isp], + get_const_field(coords_eval), + get_const_field(neutrals_density_spline_x_coeff)); + + // compute laplacian + DBSFieldMemX gradx_neutrals_density_spline_x_coeff( + get_spline_idx_range(m_spline_x_builder)); + + m_spline_x_builder( + get_field(gradx_neutrals_density_spline_x_coeff), + get_const_field(gradx_neutrals_density[isp])); + + m_spline_x_evaluator + .deriv(laplx_neutrals_density[isp], + get_const_field(coords_eval), + get_const_field(gradx_neutrals_density_spline_x_coeff)); + }); + + // build rhs of diffusive model equation + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + idx_range_fluidspx, + KOKKOS_LAMBDA(IdxSpX const ifspx) { + dn(ifspx, ineutral_density) + = -gradx_density_equilibrium_velocity(ifspx) + + gradx_diffusion_temperature(ifspx) * gradx_neutrals_density(ifspx) + + diffusion_temperature(ifspx) * laplx_neutrals_density(ifspx); + }); // density source is not solved here, we only solve transport. +} + +DFieldSpMomX DiffusiveNeutralSolver::operator()( + DFieldSpMomX const neutrals, + DConstFieldSpXVx const allfdistribu, + DConstFieldX const efield, + double const dt) const +{ + Kokkos::Profiling::pushRegion("DiffusiveNeutralSolver"); + RK2 timestepper(get_idx_range(neutrals)); + + // moments computation + IdxRangeSpX idx_range_kspx(get_idx_range(allfdistribu)); + DFieldMemSpX density_alloc(idx_range_kspx); + DFieldMemSpX velocity_alloc(idx_range_kspx); + DFieldMemSpX temperature_alloc(idx_range_kspx); + + DFieldSpX density = get_field(density_alloc); + DFieldSpX velocity = get_field(velocity_alloc); + DFieldSpX temperature = get_field(temperature_alloc); + + DConstFieldVx quadrature_coeffs = m_quadrature_coeffs; + + IdxRangeVx const idx_range_vx(get_idx_range(allfdistribu)); + + // fluid moments computation + ddc::parallel_fill(density, 0.); + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + idx_range_kspx, + KOKKOS_LAMBDA(IdxSpX const ispx) { + double particle_flux(0); + double momentum_flux(0); + for (IdxVx const ivx : idx_range_vx) { + CoordVx const coordv = ddc::coordinate(ivx); + double const val(quadrature_coeffs(ivx) * allfdistribu(ispx, ivx)); + density(ispx) += val; + particle_flux += val * coordv; + momentum_flux += val * coordv * coordv; + } + velocity(ispx) = particle_flux / density(ispx); + temperature(ispx) + = (momentum_flux - particle_flux * velocity(ispx)) / density(ispx); + }); + + timestepper.update(neutrals, dt, [&](DFieldSpMomX dn, DConstFieldSpMomX n) { + get_derivative(dn, n, density, velocity, temperature); + }); + Kokkos::Profiling::popRegion(); + return neutrals; +} diff --git a/src/geometryXVx/geometryMX/fluidtransportsolver/diffusiveneutralsolver.hpp b/src/geometryXVx/geometryMX/fluidtransportsolver/diffusiveneutralsolver.hpp new file mode 100644 index 000000000..9f2dd0eb1 --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidtransportsolver/diffusiveneutralsolver.hpp @@ -0,0 +1,137 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#include "geometry.hpp" +#include "ifluidtransportsolver.hpp" +#include "ireactionrate.hpp" + +/** + * @brief A class that solves a so-called "pressure-diffusive" fluid neutral model. + * + * The equation of the model that describes the evolution of the density of + * neutrals can be written in dimensional units as + * + * @f$\partial_t n_n + \partial_x (n_{n,eq} u_i - D_p T_n \partial_x n_n) = S_n, @f$ + * + * where @f$n_n(x,t)@f$ is the time and space dependent neutral density, @f$T_n@f$ is the + * temperature of neutrals (considered constant) and @f$u_i(x)@f$ is the ion fluid velocity. + * + * In the above equation the following definitions are used: + * + * @f$n_{n,eq} = \frac{n_i n_e K_r + n_n n_i K_{cx}}{n_i K_{cx} + n_e K_i}@f$ + * + * and + * + * @f$D_p = \frac{1}{m_n (n_i K_{cx} + n_e K_i)}@f$ + * + * where @f$n_i@f$ (resp. @f$n_e@f$) is the ion (resp. electron) density and @f$m_n@f$ stands + * for the mass of neutrals. The @f$K_i@f$, @f$K_r@f$ and @f$K_{cx}@f$ coefficients + * represent the reaction rates of ionization, recombination and charge-exchange reactions. + * + * The density source term @f$S_n@f$ is + * + * @f$S_n = n_i n_e K_r - n_n n_e K_i.@f$ + * + * The pressure-diffusive equation is normalized to the relevant normalization quantities + * of the geometryXVx folder: + * - densities to a reference density @f$n_0@f$; + * - temperatures to a reference temperature @f$T_0@f$; + * - time normalized to the electron plasma frequency @f$\omega_{pe0} = \sqrt{n_0 e^2/(m_e \varepsilon_0)}@f$; + * - space to the Debye length @f$\lambda_{D0} = \sqrt{\varepsilon_0 T_0 / (n_0 e^2)}@f$; + * - ion mean velocity to the ion thermal velocity @f$v_{Ti0} = \sqrt{T_0/m_i}@f$; + * - reaction rates to a reference rate @f$K_0@f$; + * - masses to the electron mass @f$m_e@f$. + * + * With these conventions the pressure-diffusive equation can be written with all quantities + * normalized as + * + * @f$\partial_t n_n + \partial_x (\sqrt{\frac{m_e}{m_i}}n_{n,eq} u_i - \alpha_0 D_p T_n \partial_x n_n) = \alpha_0^{-1} S_n, @f$ + * + * Where @f$\alpha_0@f$ is a normalization coefficient equal to @f$\alpha_0 = \omega_{pe0}/(n_0 K_0)@f$. + * All the terms that appear in this normalized equation keep the same expression as when writing + * the dimensional form of the model, except that quantities involved are normalized. + * + * The pressure-diffusive model is solved using a RK2 time integrator. + * Spatial derivatives are computed using splines polynomials. + */ +class DiffusiveNeutralSolver : public IFluidTransportSolver +{ +private: + IReactionRate const& m_charge_exchange; + IReactionRate const& m_ionization; + IReactionRate const& m_recombination; + + double const m_normalization_coeff; + + SplineXBuilder_1d const& m_spline_x_builder; + SplineXEvaluator_1d const& m_spline_x_evaluator; + + DConstFieldVx const m_quadrature_coeffs; + + IdxSp find_ion(IdxRangeSp const idx_range_kinsp) const; + +public: + /** + * @brief Creates an instance of the DiffusiveNeutralSolver class. + * @param[in] charge_exchange An object that represents charge-exchange reaction rate. + * @param[in] ionization An object that represents ionization reaction rate. + * @param[in] recombination An object that represents recombination reaction rate. + * @param[in] normalization_coeff A normalization coefficient for the diffusive neutral model. + * @param[in] spline_x_builder A one-dimensional spline builder. + * @param[in] spline_x_evaluator A one-dimensional spline evaluator. + * @param[in] quadrature_coeffs A constant field referencing coefficients for a quadrature. + */ + DiffusiveNeutralSolver( + IReactionRate const& charge_exchange, + IReactionRate const& ionization, + IReactionRate const& recombination, + double const normalization_coeff, + SplineXBuilder_1d const& spline_x_builder, + SplineXEvaluator_1d const& spline_x_evaluator, + DConstFieldVx const& quadrature_coeffs); + + ~DiffusiveNeutralSolver() override = default; + + /** + * @brief Updates the neutral fluid moments according to the pressure-diffusive neutral model. + * + * Within the pressure-diffusive model only the neutral density is evolved thus it is the + * only fluid moments we consider. + * + * @param[inout] neutrals The fluid moments describing the neutrals. + * @param[in] allfdistribu A constant Field referencing the distribution function. + * @param[in] efield A constant Field referencing the electric field. + * @param[in] dt The time step. + * + * @return A field referencing the neutral fluid moments passed as argument. + */ + DFieldSpMomX operator()( + DFieldSpMomX neutrals, + DConstFieldSpXVx allfdistribu, + DConstFieldX efield, + double dt) const override; + + /** + * @brief Computes the expression of the time derivative of the neutral fluid moments. + * + * The expression of the time derivative is given by the equation of the pressure-diffusive + * neutral model, that is to say + * + * @f$\partial_t n_n = - \partial_x (n_{n,eq} u_i - D_p T_n \partial_x n_n) + S_n@f$ + * + * This function is used by the time integrator (RK2 for instance). + * + * @param[inout] dn The time derivative of neutral fluid moments. + * @param[in] n The fluid moments of the neutral species. + * @param[in] density The plasma density (for ion and electrons). + * @param[in] velocity The plasma mean velocity (for ion and electrons). + * @param[in] temperature The plasma temperature (for ion and electrons). + */ + void get_derivative( + DFieldSpMomX dn, + DConstFieldSpMomX n, + DConstFieldSpX density, + DConstFieldSpX velocity, + DConstFieldSpX temperature) const; +}; diff --git a/src/geometryXVx/geometryMX/fluidtransportsolver/ifluidtransportsolver.hpp b/src/geometryXVx/geometryMX/fluidtransportsolver/ifluidtransportsolver.hpp new file mode 100644 index 000000000..c65f02eeb --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidtransportsolver/ifluidtransportsolver.hpp @@ -0,0 +1,30 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#include "geometry.hpp" + +/** + * @brief An abstract class for solving the transport of a fluid model. + */ +class IFluidTransportSolver +{ +public: + virtual ~IFluidTransportSolver() = default; + + /** + * @brief Operator for solving the fluid model on one timestep. + * @param[in, out] fluid_moments On input : a field referencing the fluid species. + * On output : a field referencing the fluid species updated + * after solving the fluid model on one timestep. + * @param[in] allfdistribu A constant field referencing the distribution function. + * @param[in] efield A constant field referencing the electric field. + * @param[in] dt The timestep. + * @return a field referencing the fluid species after solving the fluid model on one timestep. + */ + virtual DFieldSpMomX operator()( + DFieldSpMomX fluid_moments, + DConstFieldSpXVx allfdistribu, + DConstFieldX efield, + double dt) const = 0; +}; diff --git a/src/geometryXVx/geometryMX/fluidtransportsolver/nullfluidsolver.cpp b/src/geometryXVx/geometryMX/fluidtransportsolver/nullfluidsolver.cpp new file mode 100644 index 000000000..8fd7b6d97 --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidtransportsolver/nullfluidsolver.cpp @@ -0,0 +1,20 @@ +// SPDX-License-Identifier: MIT + +#include "nullfluidsolver.hpp" + +NullFluidSolver::NullFluidSolver(IdxRangeSp const& idx_range_fluidsp) +{ + // charged fluid species is not allowed for now + for (IdxSp const isp : idx_range_fluidsp) { + assert(charge(isp) == 0.); + } +} + +DFieldSpMomX NullFluidSolver::operator()( + DFieldSpMomX const fluid_moments, + DConstFieldSpXVx const allfdistribu, + DConstFieldX const efield, + double const dt) const +{ + return fluid_moments; +} diff --git a/src/geometryXVx/geometryMX/fluidtransportsolver/nullfluidsolver.hpp b/src/geometryXVx/geometryMX/fluidtransportsolver/nullfluidsolver.hpp new file mode 100644 index 000000000..709f05469 --- /dev/null +++ b/src/geometryXVx/geometryMX/fluidtransportsolver/nullfluidsolver.hpp @@ -0,0 +1,38 @@ +// SPDX-License-Identifier: MIT +#pragma once +#include "ddc_aliases.hpp" +#include "geometry.hpp" +#include "ifluidtransportsolver.hpp" + +/** + * @brief A dommy class that solves a fluid model. + * The fluid model leaves the moments of the fluid species unchanged. + */ +class NullFluidSolver : public IFluidTransportSolver +{ +public: + /** + * @brief The constructor for the class. + * + * @param[in] idx_range_fluidsp The moments index range on which the fluid species is defined. + */ + NullFluidSolver(IdxRangeSp const& idx_range_fluidsp); + + ~NullFluidSolver() override = default; + + /** + * @brief Solves a dummy fluid model on a timestep dt. + * @param[in, out] fluid_moments On input : a field referencing the moments of the fluid species. + * On output : a field referencing the moments of the fluid species + * updated after solving the dummy fluid model. + * @param[in] allfdistribu A constant field referencing the distribution function. + * @param[in] efield A constant field referencing the electric field. + * @param[in] dt The timestep. + * @return a field referencing the fluid species after solving the dummy fluid model on one timestep. + */ + DFieldSpMomX operator()( + DFieldSpMomX fluid_moments, + DConstFieldSpXVx allfdistribu, + DConstFieldX efield, + double dt) const override; +}; diff --git a/src/geometryXVx/geometryMX/kineticfluidcoupling/CMakeLists.txt b/src/geometryXVx/geometryMX/kineticfluidcoupling/CMakeLists.txt new file mode 100644 index 000000000..75ca3edcc --- /dev/null +++ b/src/geometryXVx/geometryMX/kineticfluidcoupling/CMakeLists.txt @@ -0,0 +1,30 @@ +# SPDX-License-Identifier: MIT + +foreach(GEOMETRY_VARIANT IN LISTS GEOMETRY_XVx_VARIANTS_LIST) + +add_library("fluidrhs_${GEOMETRY_VARIANT}" STATIC + kinetic_fluid_coupling_source.cpp +) + +target_include_directories("fluidrhs_${GEOMETRY_VARIANT}" + PUBLIC "${CMAKE_CURRENT_SOURCE_DIR}" +) + +target_link_libraries("fluidrhs_${GEOMETRY_VARIANT}" + PUBLIC + DDC::DDC + DDC::PDI_Wrapper + sll::SLL + gslx::geometry_${GEOMETRY_VARIANT} + gslx::quadrature + gslx::speciesinfo + gslx::initialization_${GEOMETRY_VARIANT} + gslx::reactionrates_${GEOMETRY_VARIANT} + gslx::timestepper + gslx::utils_${GEOMETRY_VARIANT} + gslx::utils +) + +add_library("gslx::fluidrhs_${GEOMETRY_VARIANT}" ALIAS "fluidrhs_${GEOMETRY_VARIANT}") + +endforeach() diff --git a/src/geometryXVx/geometryMX/kineticfluidcoupling/README.md b/src/geometryXVx/geometryMX/kineticfluidcoupling/README.md new file mode 100644 index 000000000..56b3bd8dd --- /dev/null +++ b/src/geometryXVx/geometryMX/kineticfluidcoupling/README.md @@ -0,0 +1,6 @@ +# Kinetic fluid coupling (MX) + +The `kineticfluidcoupling` folder contains code that allows for the coupling between the fluid equation of neutrals and the kinetic Boltzmann equation of plasma particles. This link is made adding two source terms that introduce or remove particles from both systems in identical and opposite quantities. + +The currently implemented coupler is : +- KineticFluidCouplingSource \ No newline at end of file diff --git a/src/geometryXVx/geometryMX/kineticfluidcoupling/ikineticfluidcoupling.hpp b/src/geometryXVx/geometryMX/kineticfluidcoupling/ikineticfluidcoupling.hpp new file mode 100644 index 000000000..29c7064b5 --- /dev/null +++ b/src/geometryXVx/geometryMX/kineticfluidcoupling/ikineticfluidcoupling.hpp @@ -0,0 +1,37 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#include "geometry.hpp" + +/** + * @brief An abstract class representing a source for both the Boltzmann and neutral fluid equations. +**/ +class IKineticFluidCoupling +{ +public: + virtual ~IKineticFluidCoupling() = default; + + /** + * @brief Operator for applying the source term on the distribution function and neutral density. + * + * The source @f$S@f$ acts on the distribution function following the + * evolution equation @f$df/dt = S_{n,N}(x) * S_v(x,v)@f$ where + * @f$S_{n,N}(x) = n_N(x) n_e(x) K_i(x) - n_i(x) n_e(x) K_r(x)@f$ + * @f$S_v(x,v)@f$ is the sum of order 0 to 2 Hermite polynomials times a Maxwellian velocity distribution function. + * + * The source @f$S@f$ acts on the neutral density following the + * evolution equation @f$dn_N/dt = - S_n,N(x)@f$ + * + * @param[in, out] allfdistribu On input: the initial value of the distribution function. + * On output: the value of the distribution function after solving + * the source evolution equation on one timestep. + * @param[in, out] neutrals On input: the initial value of the neutral density. + * On output: the value of the neutral density after solving + * the source evolution equation on one timestep. + * @param[in] dt The timestep. + * + */ + virtual void operator()(DFieldSpXVx const allfdistribu, DFieldSpMomX neutrals, double const dt) + const = 0; +}; diff --git a/src/geometryXVx/geometryMX/kineticfluidcoupling/kinetic_fluid_coupling_source.cpp b/src/geometryXVx/geometryMX/kineticfluidcoupling/kinetic_fluid_coupling_source.cpp new file mode 100644 index 000000000..b93268f02 --- /dev/null +++ b/src/geometryXVx/geometryMX/kineticfluidcoupling/kinetic_fluid_coupling_source.cpp @@ -0,0 +1,229 @@ +#include + +#include "kinetic_fluid_coupling_source.hpp" +#include "rk2.hpp" +#include "species_info.hpp" +#include "trapezoid_quadrature.hpp" + +KineticFluidCouplingSource::KineticFluidCouplingSource( + double const density_coupling_coeff, + double const momentum_coupling_coeff, + double const energy_coupling_coeff, + IReactionRate const& ionization, + IReactionRate const& recombination, + double const normalization_coeff, + DConstFieldVx const& quadrature_coeffs) // for kinetic species + : m_density_coupling_coeff(density_coupling_coeff) + , m_momentum_coupling_coeff(momentum_coupling_coeff) + , m_energy_coupling_coeff(energy_coupling_coeff) + , m_ionization(ionization) + , m_recombination(recombination) + , m_normalization_coeff(normalization_coeff) + , m_quadrature_coeffs(quadrature_coeffs) +{ + ddc::expose_to_pdi( + "kinetic_fluid_coupling_source_density_coupling_coeff", + m_density_coupling_coeff); + ddc::expose_to_pdi( + "kinetic_fluid_coupling_source_momentum_coupling_coeff", + m_momentum_coupling_coeff); + ddc::expose_to_pdi( + "kinetic_fluid_coupling_source_energy_coupling_coeff", + m_energy_coupling_coeff); +} + +IdxSp KineticFluidCouplingSource::find_ion(IdxRangeSp const dom_kinsp) const +{ + bool ion_found = false; + IdxSp iion; + for (IdxSp const isp : dom_kinsp) { + if (charge(isp) > 0) { + ion_found = true; + iion = isp; + } + } + if (!ion_found) { + throw std::runtime_error("ion not found"); + } + assert(dom_kinsp.size() == 2); + + return iion; +} + +void KineticFluidCouplingSource::get_source_term( + DFieldX density_source_neutral, + DConstFieldSpX kinsp_density, + DConstFieldSpMomX neutrals, + DConstFieldSpX ionization, + DConstFieldSpX recombination) const +{ + IdxSp const iion(find_ion(get_idx_range(kinsp_density))); + // Neutrals density source computation + IdxRangeSpMom const dom_msp(get_idx_range(neutrals)); + IdxSpMom ineutral(dom_msp.front()); + IdxRangeSp const dom_sp(get_idx_range(neutrals)); + IdxSp ispneutral(dom_sp.front()); + + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + get_idx_range(density_source_neutral), + KOKKOS_LAMBDA(IdxX const ix) { + density_source_neutral(ix) = neutrals(ineutral, ix) * kinsp_density(ielec(), ix) + * ionization(ispneutral, ix) + - kinsp_density(iion, ix) * kinsp_density(ielec(), ix) + * recombination(ispneutral, ix); + }); +} + +void KineticFluidCouplingSource::get_derivative_neutrals( + DFieldSpMomX dn, + DConstFieldSpMomX neutrals, + DConstFieldX density_source_neutral) const +{ + // neutrals dn computation + IdxRangeSpX dom_fluidspx(get_idx_range(neutrals)); + + // compute diffusive model equation terms + IdxMom const ineutral_density(0); + double const normalization_coeff_alpha0(m_normalization_coeff); + + // build rhs of diffusive model equation + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + dom_fluidspx, + KOKKOS_LAMBDA(IdxSpX const ifspx) { + IdxX const ix(ifspx); + dn(ifspx, ineutral_density) + = -density_source_neutral(ix) / normalization_coeff_alpha0; + }); +} + +void KineticFluidCouplingSource::get_derivative_allfdistribu( + DFieldSpXVx df, + DConstFieldSpXVx allfdistribu, + DConstFieldSpXVx velocity_shape_source) const +{ + // df computation + IdxRangeSpXVx dom_kspx(get_idx_range(allfdistribu)); + + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + dom_kspx, + KOKKOS_LAMBDA(IdxSpXVx const ispxvx) { df(ispxvx) = velocity_shape_source(ispxvx); }); +} + +void KineticFluidCouplingSource::operator()( + DFieldSpXVx const allfdistribu, + DFieldSpMomX neutrals, + double const dt) const +{ + Kokkos::Profiling::pushRegion("KineticFluidCouplingSource"); + RK2 timestepper_neutrals(get_idx_range(neutrals)); + RK2 timestepper_kinetic(get_idx_range(allfdistribu)); + + // useful params and index ranges + IdxSp const iion(find_ion(get_idx_range(allfdistribu))); + + // kinetic species fluid moments computation + IdxRangeSpX dom_kspx(get_idx_range(allfdistribu)); + DFieldMemSpX kinsp_density_alloc(dom_kspx); + DFieldMemSpX kinsp_velocity_alloc(dom_kspx); + DFieldMemSpX kinsp_temperature_alloc(dom_kspx); + + DFieldSpX kinsp_density = get_field(kinsp_density_alloc); + DFieldSpX kinsp_velocity = get_field(kinsp_velocity_alloc); + DFieldSpX kinsp_temperature = get_field(kinsp_temperature_alloc); + + DConstFieldVx quadrature_coeffs = get_const_field(m_quadrature_coeffs); + + IdxRangeVx const idx_range_vx(get_idx_range(allfdistribu)); + + ddc::parallel_fill(Kokkos::DefaultExecutionSpace(), kinsp_density, 0.); + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + dom_kspx, + KOKKOS_LAMBDA(IdxSpX const ispx) { + double particle_flux(0); + double momentum_flux(0); + for (IdxVx const ivx : idx_range_vx) { + CoordVx const coordv = ddc::coordinate(ivx); + double const val(quadrature_coeffs(ivx) * allfdistribu(ispx, ivx)); + kinsp_density(ispx) += val; + particle_flux += val * coordv; + momentum_flux += val * coordv * coordv; + } + kinsp_velocity(ispx) = particle_flux / kinsp_density(ispx); + kinsp_temperature(ispx) = (momentum_flux - particle_flux * kinsp_velocity(ispx)) + / kinsp_density(ispx); + }); + + // building reaction rates + IdxRangeSpX dom_fluidspx(get_idx_range(neutrals)); + + DFieldMemSpX ionization_rate_alloc(dom_fluidspx); + DFieldMemSpX recombination_rate_alloc(dom_fluidspx); + + DFieldSpX ionization_rate = get_field(ionization_rate_alloc); + DFieldSpX recombination_rate = get_field(recombination_rate_alloc); + + m_ionization(ionization_rate, kinsp_density, kinsp_temperature); + m_recombination(recombination_rate, kinsp_density, kinsp_temperature); + + // source term computation + IdxRangeX grid_x(get_idx_range(allfdistribu)); + + DFieldMemX density_source_neutral_alloc(grid_x); + auto density_source_neutral = get_field(density_source_neutral_alloc); + get_source_term( + density_source_neutral, + kinsp_density, + neutrals, + ionization_rate, + recombination_rate); + + // S(v) velocity shape calculation for kinetic species + DFieldMemSpXVx velocity_shape_source_alloc(get_idx_range(allfdistribu)); + DFieldSpXVx velocity_shape_source = get_field(velocity_shape_source_alloc); + + double density_coupling_coeff_proxy = m_density_coupling_coeff; + double momentum_coupling_coeff_proxy = m_momentum_coupling_coeff; + double energy_coupling_coeff_proxy = m_energy_coupling_coeff; + double const normalization_coeff_alpha0_proxy = m_normalization_coeff; + + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + get_idx_range(allfdistribu), + KOKKOS_LAMBDA(IdxSpXVx const ispxvx) { + IdxX const ix(ispxvx); + IdxVx const ivx(ispxvx); + CoordVx const coordvx = ddc::coordinate(ivx); + double const neutral_temperature + = (kinsp_temperature(iion, ix) + kinsp_temperature(ielec(), ix)) / 2.; + + double const coordvx_sq = coordvx * coordvx; + double const density_source + = density_coupling_coeff_proxy + * (1.5 - coordvx_sq / (2 * neutral_temperature)) + * Kokkos::exp(-coordvx_sq / (2 * neutral_temperature)); + double const momentum_source + = momentum_coupling_coeff_proxy * Kokkos::sqrt(2 / neutral_temperature) + * coordvx * Kokkos::exp(-coordvx_sq / (2 * neutral_temperature)); + double const energy_source = 2 * energy_coupling_coeff_proxy + * (-1 + coordvx_sq / neutral_temperature) + * Kokkos::exp(-coordvx_sq / (2 * neutral_temperature)); + velocity_shape_source(ispxvx) = (density_source_neutral(ix) + / (Kokkos::sqrt(2 * M_PI * neutral_temperature) + * normalization_coeff_alpha0_proxy)) + * density_source + + momentum_source + energy_source; + }); + + timestepper_kinetic.update(allfdistribu, dt, [&](DFieldSpXVx df, DConstFieldSpXVx f) { + get_derivative_allfdistribu(df, f, velocity_shape_source); + }); + timestepper_neutrals.update(neutrals, dt, [&](DFieldSpMomX dn, DConstFieldSpMomX n) { + get_derivative_neutrals(dn, n, density_source_neutral); + }); + + Kokkos::Profiling::popRegion(); +} diff --git a/src/geometryXVx/geometryMX/kineticfluidcoupling/kinetic_fluid_coupling_source.hpp b/src/geometryXVx/geometryMX/kineticfluidcoupling/kinetic_fluid_coupling_source.hpp new file mode 100644 index 000000000..ce24b2edb --- /dev/null +++ b/src/geometryXVx/geometryMX/kineticfluidcoupling/kinetic_fluid_coupling_source.hpp @@ -0,0 +1,124 @@ +// SPDX-License-Identifier: MIT +#pragma once +#include + +#include "ddc_aliases.hpp" +#include "geometry.hpp" +#include "ikineticfluidcoupling.hpp" +#include "ireactionrate.hpp" + +/** + * @brief A class that describes a source of particles due to neutrals. + * + * The KineticFluidCouplingSource class solves the following evolution equations: + * @f$df/dt = S_n,N(x) * S_v(x,v)@f$ + * where @f$S_n,N(x)@f$ is what we call the density_source_neutral + * @f$dn_N/dt = - S_n,N(x)@f$ + * Where @f$S_n,N(x) = n_N(x) n_e(x) K_i(x) - n_i(x) n_e(x) K_r(x)@f$ + * @f$S_v(x,v)@f$ is the sum of order 0 to 2 Hermite polynomials times a Maxwellian velocity distribution function. + * + * + * The velocity_shape_source @f$S_v(x,v)@f$ defines the velocity profile of the source in the parallel velocity direction. + * It is the sum of a source that injects only density, a source that injects only momentum and a source that injects only energy. + * If the density and energy parameters are equal to one (usual case), the resulting velocity_shape is maxwellian. + * + * The complete description of the operator can be found in [rhs docs](https://github.com/gyselax/gyselalibxx/blob/main/doc/geometryXVx/kinetic_source.pdf). + */ +class KineticFluidCouplingSource : public IKineticFluidCoupling +{ +private: + double m_density_coupling_coeff; + double m_momentum_coupling_coeff; + double m_energy_coupling_coeff; + IReactionRate const& m_ionization; + IReactionRate const& m_recombination; + double m_normalization_coeff; + DConstFieldVx const m_quadrature_coeffs; + +public: + /** + * @brief Creates an instance of the KineticFluidCouplingSource class. + * + * @param[in] density_coupling_coeff The coefficient of the density source. + * @param[in] momentum_coupling_coeff The coefficient of the momentum source. + * @param[in] energy_coupling_coeff The coefficient of the energy source. + * @param[in] ionization The rate of the ionization reaction. + * @param[in] recombination The rate of the recombination reaction. + * @param[in] normalization_coeff The normalization coefficient of neutrals. + * @param[in] quadrature_coeffs A constant field referencing coefficients for a quadrature. + */ + KineticFluidCouplingSource( + double density_coupling_coeff, + double momentum_coupling_coeff, + double energy_coupling_coeff, + IReactionRate const& ionization, + IReactionRate const& recombination, + double normalization_coeff, + DConstFieldVx const& quadrature_coeffs); + + ~KineticFluidCouplingSource() override = default; + + /** + * @brief Update the distribution function and neutral density following the KineticFluidCouplingSource operator. + * + * @param[in, out] allfdistribu The distribution function. + * @param[in, out] neutrals The neutral density. + * @param[in] dt The time step over which the collisions occur. + * + */ + void operator()(DFieldSpXVx const allfdistribu, DFieldSpMomX neutrals, double const dt) + const override; + +public: + /** + * @brief Returns the index of the ion species in the index range. + * + * @param[in] idx_range_kinsp The index range of the kinetic species. + * + * @return The index of the ion species in the index range. + */ + IdxSp find_ion(IdxRangeSp const idx_range_kinsp) const; + + /** + * @brief Computes the source term density_source_neutral(x) of the KineticFluidCouplingSource operator. + * + * @param[in, out] density_source_neutral The source term. + * @param[in] kinsp_density The computed plasma densities of the distribution function. + * @param[in] neutrals The neutral density. + * @param[in] ionization The ionization rate. + * @param[in] recombination The recombination rate. + * + */ + void get_source_term( + DFieldX density_source_neutral, + DConstFieldSpX kinsp_density, + DConstFieldSpMomX neutrals, + DConstFieldSpX ionization, + DConstFieldSpX recombination) const; + + /** + * @brief Computes dn (of neutral density) for the equation dn/dt = - density_source_neutral. + * + * @param[in, out] dn The infinitesimal of the neutral density. + * @param[in] neutrals The neutral density. + * @param[in] density_source_neutral The density source term. + * + */ + void get_derivative_neutrals( + DFieldSpMomX dn, + DConstFieldSpMomX neutrals, + DConstFieldX density_source_neutral) const; + + /** + * @brief Computes df for the equation df/dt = density_source_neutral(x) * velocity_shape_source(x,v). + * + * @param[in, out] df The infinitesimal of the distribution function. + * @param[in] allfdistribu The distribution function. + * @param[in] velocity_shape_source The velocity shape of the source. + * + */ + void get_derivative_allfdistribu( + DFieldSpXVx df, + DConstFieldSpXVx allfdistribu, + DConstFieldSpXVx velocity_shape_source) const; +}; diff --git a/src/geometryXVx/geometryMX/reactionrates/CMakeLists.txt b/src/geometryXVx/geometryMX/reactionrates/CMakeLists.txt new file mode 100644 index 000000000..24350dded --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/CMakeLists.txt @@ -0,0 +1,29 @@ +# SPDX-License-Identifier: MIT + +foreach(GEOMETRY_VARIANT IN LISTS GEOMETRY_XVx_VARIANTS_LIST) + +add_library("reactionrates_${GEOMETRY_VARIANT}" STATIC + constantrate.cpp + charge_exchange.cpp + ionization.cpp + recombination.cpp +) + +target_include_directories("reactionrates_${GEOMETRY_VARIANT}" + PUBLIC "${CMAKE_CURRENT_SOURCE_DIR}" +) + +target_link_libraries("reactionrates_${GEOMETRY_VARIANT}" + PUBLIC + DDC::DDC + DDC::PDI_Wrapper + sll::SLL + gslx::geometry_${GEOMETRY_VARIANT} + gslx::speciesinfo + gslx::utils + +) + +add_library("gslx::reactionrates_${GEOMETRY_VARIANT}" ALIAS "reactionrates_${GEOMETRY_VARIANT}") + +endforeach() diff --git a/src/geometryXVx/geometryMX/reactionrates/README.md b/src/geometryXVx/geometryMX/reactionrates/README.md new file mode 100644 index 000000000..1396d4c68 --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/README.md @@ -0,0 +1,10 @@ +# Reaction rates + +The `reactionrates` folder contains all the code describing reactions within the `geometryMX` framework. + +The interface IReactionRates describes reaction rate that depend on density and temperature. +Existing reaction rates that implements such interface are: +- ConstantRate +- ChargeExchange +- Ionization +- Recombination \ No newline at end of file diff --git a/src/geometryXVx/geometryMX/reactionrates/charge_exchange.cpp b/src/geometryXVx/geometryMX/reactionrates/charge_exchange.cpp new file mode 100644 index 000000000..cdd079a77 --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/charge_exchange.cpp @@ -0,0 +1,59 @@ +// SPDX-License-Identifier: MIT + +#include + +#include "charge_exchange.hpp" +#include "ratecomputation.hpp" +#include "species_info.hpp" + +ChargeExchangeRate::ChargeExchangeRate(double const norm_coeff_rate) + : m_cx_coefficients("chargexchange_coefficients") + , m_norm_coeff_rate(norm_coeff_rate) +{ + double cx_coefficients_alloc[s_coefficients_size] + = {0.25125030648153424, + 0.37349850950319474, + -0.009966677207985306, + 0.017922185310747015, + -0.010699854255929037}; + + DKokkosView_h cx_coefficients_host(cx_coefficients_alloc); + Kokkos::deep_copy(m_cx_coefficients, cx_coefficients_host); + PDI_multi_expose( + "cx_rate_coeff_pol_expose", + "charge_exchange_coefficients", + cx_coefficients_host.data(), + PDI_OUT, + NULL); +} + +IdxSp find_ion(IdxRangeSp const idx_range_kinsp) +{ + bool ion_found = false; + IdxSp iion; + for (IdxSp const isp : idx_range_kinsp) { + if (charge(isp) > 0.) { + ion_found = true; + iion = isp; + } + } + if (!ion_found) { + throw std::runtime_error("ion not found"); + } + assert(idx_range_kinsp.size() == 2); + + return iion; +} + +DFieldSpX ChargeExchangeRate::operator()( + DFieldSpX rate, + DConstFieldSpX density, + DConstFieldSpX temperature) const +{ + return detail::compute_rate_ion_temperature( + Kokkos::DefaultExecutionSpace(), + rate, + temperature, + m_cx_coefficients, + m_norm_coeff_rate); +} diff --git a/src/geometryXVx/geometryMX/reactionrates/charge_exchange.hpp b/src/geometryXVx/geometryMX/reactionrates/charge_exchange.hpp new file mode 100644 index 000000000..83612c51c --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/charge_exchange.hpp @@ -0,0 +1,47 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#include "geometry.hpp" +#include "ireactionrate.hpp" + +/** + * @brief A class that describes a charge-exchange reaction rate. + */ +class ChargeExchangeRate : public IReactionRate +{ +private: + /* + * @brief Stores the linear coefficients to compute the polynomial for the charge-exchange reaction rate vs. ion temperature. + */ + static constexpr std::size_t s_coefficients_size = 5; + DKokkosView m_cx_coefficients; + double const m_norm_coeff_rate; + +public: + /** + * @brief Creates an instance of the ConstantChargeExchangeRate class. + * A polynomial of reaction rate vs. ion temperature is fitted in log-log space. + * The polynomial fits data from the OPEN-ADAS database for Hydrogen. + * + * @param[in] norm_coeff_rate All rate coefficients coefficients are normalized so that CX is + * of order unity at normalized density (n) = 1 and normalized temperature (T) = 1 + * with n_0 = 1e20 and T_0 = 10 eV. + * These are typical values for a SOL plasma. + * The norm_coeff_rate parameter shifts all the reaction rates to modify the source dynamics. + */ + explicit ChargeExchangeRate(double norm_coeff_rate); + + ~ChargeExchangeRate() override = default; + + /** + * @brief Compute the charge-exchange reaction rate depending on density and temperature. + * + * @param[out] rate The charge-exchange reaction rates. + * @param[in] density The plasma density at which the reaction rate is computed. Although inputted, charge-exchange reaction rate is not affected by density. + * @param[in] temperature The plasma temperature at which the reaction rate is computed. + * @return The charge-exchange reaction rate. + */ + DFieldSpX operator()(DFieldSpX rate, DConstFieldSpX density, DConstFieldSpX temperature) + const override; +}; diff --git a/src/geometryXVx/geometryMX/reactionrates/constantrate.cpp b/src/geometryXVx/geometryMX/reactionrates/constantrate.cpp new file mode 100644 index 000000000..dc9b5c601 --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/constantrate.cpp @@ -0,0 +1,14 @@ +// SPDX-License-Identifier: MIT + +#include "constantrate.hpp" + +ConstantRate::ConstantRate(double const value) : m_rate_value(value) {} + +DFieldSpX ConstantRate::operator()( + DFieldSpX rate, + DConstFieldSpX density, + DConstFieldSpX temperature) const +{ + ddc::parallel_fill(rate, m_rate_value); + return rate; +} diff --git a/src/geometryXVx/geometryMX/reactionrates/constantrate.hpp b/src/geometryXVx/geometryMX/reactionrates/constantrate.hpp new file mode 100644 index 000000000..ea0b39676 --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/constantrate.hpp @@ -0,0 +1,35 @@ +// SPDX-License-Identifier: MIT +#pragma once + +#include "geometry.hpp" +#include "ireactionrate.hpp" + +/** + * @brief A class that describes a reaction rate that is constant. + */ +class ConstantRate : public IReactionRate +{ +private: + double const m_rate_value; + +public: + /** + * @brief Creates an instance of the ConstantRate class. + * @param[in] value The constant value of the reaction rate. + */ + ConstantRate(double const value); + + ~ConstantRate() override = default; + + /** + * @brief Operator for computing the reaction rate. + * + * @param[out] rate On input: the uninitialized value of a Field referencing a reaction rate. + * On output: the field referencing a constant reaction rate. + * @param[in] density A field referencing the density. + * @param[in] temperature A field referencing the temperatures. + * @return A field referencing the reaction rate. + */ + DFieldSpX operator()(DFieldSpX rate, DConstFieldSpX density, DConstFieldSpX temperature) + const override; +}; diff --git a/src/geometryXVx/geometryMX/reactionrates/ionization.cpp b/src/geometryXVx/geometryMX/reactionrates/ionization.cpp new file mode 100644 index 000000000..69193a2a7 --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/ionization.cpp @@ -0,0 +1,55 @@ +// SPDX-License-Identifier: MIT + +#include "ionization.hpp" +#include "ratecomputation.hpp" + +IonizationRate::IonizationRate(double const norm_coeff_rate) + : m_slope_coefficient("slope_coefficient") + , m_intercept_coefficient("intercept_coefficient") + , m_norm_coeff_rate(norm_coeff_rate) +{ + double slope_coefficient_alloc[s_coefficients_size] + = {0.06478416786452716, + -0.06283835812957501, + 0.0533047026400489, + -0.02412714188219726, + 0.005377140897108906, + -0.00047180128893166466}; + double intercept_coefficient_alloc[s_coefficients_size] + = {0.053216546399122204, + 1.4939944926753081, + -1.8156125022306027, + 1.269858057577872, + -0.468107496181505, + 0.06406763661421713}; + + DKokkosView_h slope_coefficient_host(slope_coefficient_alloc); + DKokkosView_h intercept_coefficient_host(intercept_coefficient_alloc); + Kokkos::deep_copy(m_slope_coefficient, slope_coefficient_host); + Kokkos::deep_copy(m_intercept_coefficient, intercept_coefficient_host); + + PDI_multi_expose( + "i_rate_coeff_pol_expose", + "ionization_slope_coefficients", + slope_coefficient_host.data(), + PDI_OUT, + "ionization_intercept_coefficients", + intercept_coefficient_host.data(), + PDI_OUT, + NULL); +} + +DFieldSpX IonizationRate::operator()( + DFieldSpX rate, + DConstFieldSpX density, + DConstFieldSpX temperature) const +{ + return detail::compute_rate_electron_density_temperature( + Kokkos::DefaultExecutionSpace(), + rate, + density, + temperature, + m_slope_coefficient, + m_intercept_coefficient, + m_norm_coeff_rate); +} diff --git a/src/geometryXVx/geometryMX/reactionrates/ionization.hpp b/src/geometryXVx/geometryMX/reactionrates/ionization.hpp new file mode 100644 index 000000000..ad919b76b --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/ionization.hpp @@ -0,0 +1,48 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#include "geometry.hpp" +#include "ireactionrate.hpp" + +/** + * @brief A class that describes a ionization reaction rate. + */ +class IonizationRate : public IReactionRate +{ +private: + /** + * @brief Stores the coefficients depending on electron density for calculating the ionization reaction rate polynomial as a function of electron temperature. + */ + static constexpr std::size_t s_coefficients_size = 6; + DKokkosView m_slope_coefficient; + DKokkosView m_intercept_coefficient; + + double const m_norm_coeff_rate; + +public: + /** + * @brief Creates an instance of the ConstantIonizationRate class. + * A polynomial of reaction rate vs. electron temperature is fitted. + * Coefficients are fitted in semi-log space, while the rate vs. electron temperature polynomial is fitted in log-log space. + * The polynomial fits data from the OPEN-ADAS database for Hydrogen. + * + * @param[in] norm_coeff_rate All rate coefficients are normalized so that CX is of order unity at normalized density (n) = 1 and normalized temperature (T) = 1 with n_0 = 1e20 and T_0 = 10 eV. + * These are typical values for a SOL plasma. + * The norm_coeff_rate parameter shifts all the reaction rates to modify the source dynamics. + */ + explicit IonizationRate(double norm_coeff_rate); + + ~IonizationRate() override = default; + + /** + * @brief Compute the ionization reaction rate depending on density and temperature. + * + * @param[out] rate The ionization reaction rates. + * @param[in] density The plasma density at which the reaction rate is computed. + * @param[in] temperature The plasma temperature at which the reaction rate is computed. + * @return The ionization reaction rate. + */ + DFieldSpX operator()(DFieldSpX rate, DConstFieldSpX density, DConstFieldSpX temperature) + const override; +}; diff --git a/src/geometryXVx/geometryMX/reactionrates/ireactionrate.hpp b/src/geometryXVx/geometryMX/reactionrates/ireactionrate.hpp new file mode 100644 index 000000000..392417147 --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/ireactionrate.hpp @@ -0,0 +1,27 @@ +// SPDX-License-Identifier: MIT +#pragma once + +#include + +#include "geometry.hpp" + +/** + * @brief An abstract interface representing a reaction rate that depends on temperature and density. + */ +class IReactionRate +{ +public: + virtual ~IReactionRate() = default; + + /** + * @brief Operator for computing the reaction rate from two Fields referencing density and temperature. + * + * @param[out] rate On input: the uninitialized value of a Field referencing a reaction rate. + * On output: the value of reaction rate. + * @param[in] density The density at which the reaction rate should be computed. + * @param[in] temperature The temperature at which the reaction rate should be computed. + * @return A field referencing the reaction rate. + */ + virtual DFieldSpX operator()(DFieldSpX rate, DConstFieldSpX density, DConstFieldSpX temperature) + const = 0; +}; diff --git a/src/geometryXVx/geometryMX/reactionrates/ratecomputation.hpp b/src/geometryXVx/geometryMX/reactionrates/ratecomputation.hpp new file mode 100644 index 000000000..507fc169d --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/ratecomputation.hpp @@ -0,0 +1,62 @@ +// SPDX-License-Identifier: MIT + +#pragma once +#include "ddc_alias_inline_functions.hpp" +#include "ddc_aliases.hpp" +#include "ireactionrate.hpp" + +namespace detail { + +template +DFieldSpX compute_rate_electron_density_temperature( + Kokkos::DefaultExecutionSpace exec_space, + DFieldSpX rate, + DConstFieldSpX density, + DConstFieldSpX temperature, + CoeffView slope_coefficients, + CoeffView intercept_coefficients, + double norm_coeff_rate) +{ + ddc::parallel_for_each( + exec_space, + get_idx_range(rate), + KOKKOS_LAMBDA(IdxSpX const ifspx) { + double temperature_log10 + = Kokkos::log10(temperature(ielec(), ddc::select(ifspx))); + double density_log10 = Kokkos::log10(density(ielec(), ddc::select(ifspx))); + + double rate_log10 = 0.0; + for (int i = 0; i < slope_coefficients.extent(0); ++i) { + double polynomial_cs + = slope_coefficients(i) * density_log10 + intercept_coefficients(i); + rate_log10 += polynomial_cs * Kokkos::pow(temperature_log10, i); + } + rate(ifspx) = Kokkos::pow(10, rate_log10) * norm_coeff_rate; + }); + return rate; +} + +template +DFieldSpX compute_rate_ion_temperature( + Kokkos::DefaultExecutionSpace exec_space, + DFieldSpX rate, + DConstFieldSpX temperature, + CoeffView polynomial_coefficients, + double norm_coeff_rate) +{ + ddc::parallel_for_each( + exec_space, + get_idx_range(rate), + KOKKOS_LAMBDA(IdxSpX const ifspx) { + double temperature_log10 + = Kokkos::log10(temperature(ielec(), ddc::select(ifspx))); + + double rate_log10 = 0.0; + for (int i = 0; i < polynomial_coefficients.extent(0); ++i) { + rate_log10 += polynomial_coefficients[i] * Kokkos::pow(temperature_log10, i); + } + rate(ifspx) = Kokkos::pow(10, rate_log10) * norm_coeff_rate; + }); + return rate; +} +} // namespace detail diff --git a/src/geometryXVx/geometryMX/reactionrates/recombination.cpp b/src/geometryXVx/geometryMX/reactionrates/recombination.cpp new file mode 100644 index 000000000..aacfa9004 --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/recombination.cpp @@ -0,0 +1,46 @@ +// SPDX-License-Identifier: MIT + +#include "ratecomputation.hpp" +#include "recombination.hpp" +#include "species_info.hpp" + +RecombinationRate::RecombinationRate(double const norm_coeff_rate) + : m_slope_coefficient("slope_coefficient") + , m_intercept_coefficient("intercept_coefficient") + , m_norm_coeff_rate(norm_coeff_rate) +{ + double slope_coefficient_alloc[s_coefficients_size] + = {0.03849324670136343, -0.03713312941661376}; + double intercept_coefficient_alloc[s_coefficients_size] + = {-5.117013348529228, -1.1497231886316353}; + + DKokkosView_h slope_coefficient_host(slope_coefficient_alloc); + DKokkosView_h intercept_coefficient_host(intercept_coefficient_alloc); + Kokkos::deep_copy(m_slope_coefficient, slope_coefficient_host); + Kokkos::deep_copy(m_intercept_coefficient, intercept_coefficient_host); + + PDI_multi_expose( + "r_rate_coeff_pol_expose", + "recombination_slope_coefficients", + slope_coefficient_host.data(), + PDI_OUT, + "recombination_intercept_coefficients", + intercept_coefficient_host.data(), + PDI_OUT, + NULL); +} + +DFieldSpX RecombinationRate::operator()( + DFieldSpX rate, + DConstFieldSpX density, + DConstFieldSpX temperature) const +{ + return detail::compute_rate_electron_density_temperature( + Kokkos::DefaultExecutionSpace(), + rate, + density, + temperature, + m_slope_coefficient, + m_intercept_coefficient, + m_norm_coeff_rate); +} diff --git a/src/geometryXVx/geometryMX/reactionrates/recombination.hpp b/src/geometryXVx/geometryMX/reactionrates/recombination.hpp new file mode 100644 index 000000000..42df0974e --- /dev/null +++ b/src/geometryXVx/geometryMX/reactionrates/recombination.hpp @@ -0,0 +1,48 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#include "geometry.hpp" +#include "ireactionrate.hpp" + +/** + * @brief A class that describes a recombination reaction rate. + */ +class RecombinationRate : public IReactionRate +{ +private: + /** + * @brief Stores the coefficients depending on electron density for calculating the recombination reaction rate polynomial as a function of electron temperature. + */ + static constexpr std::size_t s_coefficients_size = 2; + DKokkosView m_slope_coefficient; + DKokkosView m_intercept_coefficient; + + double const m_norm_coeff_rate; + +public: + /** + * @brief Creates an instance of the ConstantRecombinationRate class. + * A polynomial of reaction rate vs. electron temperature is fitted. + * Coefficients are fitted in semi-log space, while the rate vs. electron temperature polynomial is fitted in log-log space. + * The polynomial fits data from the OPEN-ADAS database for Hydrogen. + * + * @param[in] norm_coeff_rate All rate coefficients are normalized so that CX is of order unity at normalized density (n) = 1 and normalized temperature (T) = 1 with n_0 = 1e20 and T_0 = 10 eV. + * These are typical values for a SOL plasma. + * The norm_coeff_rate parameter shifts all the reaction rates to modify the source dynamics. + */ + explicit RecombinationRate(double norm_coeff_rate); + + ~RecombinationRate() override = default; + + /** + * @brief Compute the recombination reaction rate depending on density and temperature. + * + * @param[out] rate The recombination reaction rates. + * @param[in] density The plasma density at which the reaction rate is computed. + * @param[in] temperature The plasma temperature at which the reaction rate is computed. + * @return The recombination reaction rate. + */ + DFieldSpX operator()(DFieldSpX rate, DConstFieldSpX density, DConstFieldSpX temperature) + const override; +}; diff --git a/src/geometryXVx/time_integration_hybrid/CMakeLists.txt b/src/geometryXVx/time_integration_hybrid/CMakeLists.txt new file mode 100644 index 000000000..d18ef92f5 --- /dev/null +++ b/src/geometryXVx/time_integration_hybrid/CMakeLists.txt @@ -0,0 +1,29 @@ +# SPDX-License-Identifier: MIT + +foreach(GEOMETRY_VARIANT IN LISTS GEOMETRY_XVx_VARIANTS_LIST) + +add_library("time_integration_hybrid_${GEOMETRY_VARIANT}" STATIC + predcorr_hybrid.cpp +) + +target_include_directories("time_integration_hybrid_${GEOMETRY_VARIANT}" + PUBLIC "${CMAKE_CURRENT_SOURCE_DIR}" +) + +target_link_libraries("time_integration_hybrid_${GEOMETRY_VARIANT}" + PUBLIC + DDC::DDC + DDC::PDI_Wrapper + gslx::boltzmann_${GEOMETRY_VARIANT} + gslx::initialization_${GEOMETRY_VARIANT} + gslx::fluidsolver_${GEOMETRY_VARIANT} + gslx::fluidrhs_${GEOMETRY_VARIANT} + gslx::poisson_${GEOMETRY_VARIANT} + gslx::speciesinfo + gslx::utils + +) + +add_library("gslx::time_integration_hybrid_${GEOMETRY_VARIANT}" ALIAS "time_integration_hybrid_${GEOMETRY_VARIANT}") + +endforeach() diff --git a/src/geometryXVx/time_integration_hybrid/README.md b/src/geometryXVx/time_integration_hybrid/README.md new file mode 100644 index 000000000..08882c32c --- /dev/null +++ b/src/geometryXVx/time_integration_hybrid/README.md @@ -0,0 +1,15 @@ +# Time integration hybrid + +Code for time integrators that solves a Boltzmann-Poisson system for the electrostatic potential and the electron and ion distribution function, along with a fluid model to describe a fluid species. A predictor-corrector scheme is used to solve the Vlasov Poisson system coupled to the fluid equation on one timestep $\Delta t$ as +1. Find the electrostatic potential at time $t+\Delta t/2$ following: +- Solve Boltzmann equation for the distribution function at time $t+\Delta t/2$; +- Using this distribution function, solve Quasi-Neutrality equation for the electrostatic potential at time $t+\Delta t/2$. +2. With the potential computed at time $t+\Delta t/2$: +- Solve Boltzmann equation for the distribution function at time $t+\Delta t$; +- Using the distribution function at time $t+\Delta t$, solve Quasi-Neutrality equation for the electrostatic potential at time $t+\Delta t$; +- Solve the fluid model for the fluid species fluid moments at time $t+\Delta t$. + +For more information about the Boltzmann-Poisson time integrator, see [time\_integration](./../time_integration/README.md). + +The implemented time integrators that take into account fluid species are: +- PredCorrHybrid \ No newline at end of file diff --git a/src/geometryXVx/time_integration_hybrid/itimesolver_hybrid.hpp b/src/geometryXVx/time_integration_hybrid/itimesolver_hybrid.hpp new file mode 100644 index 000000000..16eeaa79a --- /dev/null +++ b/src/geometryXVx/time_integration_hybrid/itimesolver_hybrid.hpp @@ -0,0 +1,33 @@ +// SPDX-License-Identifier: MIT +#pragma once + +#include "geometry.hpp" + +/** + * @brief An abstract class for solving a Boltzmann-Poisson system of equations coupled to a fluid model. + */ +class ITimeSolverHybrid +{ +public: + virtual ~ITimeSolverHybrid() = default; + + /** + * @brief Operator for solving the Boltzmann-Poisson-fluid system. + * @param[in, out] allfdistribu On input : the initial value of the distribution function. + * On output : the value of the distribution function after solving + * the Boltzmann-Poisson-fluid system a given number of iterations. + * @param[in, out] fluid_moments On input : a field referencing the fluid species. + * On output : the fluid species after solving + * the Boltzmann-Poisson-fluid system a given number of iterations. + * @param[in] time_start The physical time at the start of the simulation. + * @param[in] dt The timestep. + * @param[in] steps The number of iterations to be performed by the solver. + * @return The distribution function after solving the system. + */ + virtual DFieldSpXVx operator()( + DFieldSpXVx allfdistribu, + DFieldSpMomX fluid_moments, + double time_start, + double dt, + int steps = 1) const = 0; +}; diff --git a/src/geometryXVx/time_integration_hybrid/predcorr_hybrid.cpp b/src/geometryXVx/time_integration_hybrid/predcorr_hybrid.cpp new file mode 100644 index 000000000..4f5a61075 --- /dev/null +++ b/src/geometryXVx/time_integration_hybrid/predcorr_hybrid.cpp @@ -0,0 +1,99 @@ +// SPDX-License-Identifier: MIT + +#include + +#include + +#include "iboltzmannsolver.hpp" +#include "ifluidtransportsolver.hpp" +#include "iqnsolver.hpp" +#include "predcorr_hybrid.hpp" + +PredCorrHybrid::PredCorrHybrid( + IBoltzmannSolver const& boltzmann_solver, + IFluidTransportSolver const& fluid_solver, + IQNSolver const& poisson_solver, + IKineticFluidCoupling const& kinetic_fluid_coupling) + : m_boltzmann_solver(boltzmann_solver) + , m_fluid_solver(fluid_solver) + , m_poisson_solver(poisson_solver) + , m_kinetic_fluid_coupling(kinetic_fluid_coupling) +{ +} + +DFieldSpXVx PredCorrHybrid::operator()( + DFieldSpXVx const allfdistribu, + DFieldSpMomX fluid_moments, + double const time_start, + double const dt, + int const steps) const +{ + auto allfdistribu_alloc = ddc::create_mirror_view(allfdistribu); + host_t allfdistribu_host = get_field(allfdistribu_alloc); + + IdxRangeX const idx_range_x = get_idx_range(allfdistribu); + + // electrostatic potential and electric field (depending only on x) + host_t electrostatic_potential_host(idx_range_x); + DFieldMemX electrostatic_potential(idx_range_x); + + DFieldMemX electric_field(idx_range_x); + + host_t fluid_moments_host(get_idx_range(fluid_moments)); + + // a 2D chunk of the same size as fdistribu + host_t allfdistribu_half_t_host(get_idx_range(allfdistribu)); + DFieldMemSpXVx allfdistribu_half_t(get_idx_range(allfdistribu)); + + m_poisson_solver(electrostatic_potential, electric_field, allfdistribu); + + int iter = 0; + for (; iter < steps; ++iter) { + double const iter_time = time_start + iter * dt; + + // computation of the electrostatic potential at time tn and + // the associated electric field + m_poisson_solver(electrostatic_potential, electric_field, allfdistribu); + // copies necessary to PDI + ddc::parallel_deepcopy(allfdistribu_host, allfdistribu); + ddc::parallel_deepcopy(electrostatic_potential_host, electrostatic_potential); + ddc::parallel_deepcopy(fluid_moments_host, fluid_moments); + ddc::PdiEvent("iteration") + .with("iter", iter) + .and_with("time_saved", iter_time) + .and_with("fdistribu", allfdistribu_host) + .and_with("fluid_moments", fluid_moments_host) + .and_with("electrostatic_potential", electrostatic_potential_host); + + // copy fdistribu + ddc::parallel_deepcopy(allfdistribu_half_t, allfdistribu); + + + // predictor + m_boltzmann_solver(allfdistribu_half_t, electric_field, dt / 2); + + // computation of the electrostatic potential at time tn+1/2 + // and the associated electric field + m_poisson_solver(electrostatic_potential, electric_field, allfdistribu_half_t); + // correction on a dt + m_boltzmann_solver(allfdistribu, electric_field, dt); + m_fluid_solver(fluid_moments, allfdistribu, electric_field, dt); + + m_kinetic_fluid_coupling(allfdistribu, fluid_moments, dt); + } + + double const final_time = time_start + iter * dt; + m_poisson_solver(electrostatic_potential, electric_field, allfdistribu); + + ddc::parallel_deepcopy(allfdistribu_host, allfdistribu); + ddc::parallel_deepcopy(electrostatic_potential_host, electrostatic_potential); + ddc::parallel_deepcopy(fluid_moments_host, fluid_moments); + ddc::PdiEvent("last_iteration") + .with("iter", iter) + .and_with("time_saved", final_time) + .and_with("fdistribu", allfdistribu_host) + .and_with("fluid_moments", fluid_moments_host) + .and_with("electrostatic_potential", electrostatic_potential_host); + + return allfdistribu; +} diff --git a/src/geometryXVx/time_integration_hybrid/predcorr_hybrid.hpp b/src/geometryXVx/time_integration_hybrid/predcorr_hybrid.hpp new file mode 100644 index 000000000..617908fd0 --- /dev/null +++ b/src/geometryXVx/time_integration_hybrid/predcorr_hybrid.hpp @@ -0,0 +1,73 @@ +// SPDX-License-Identifier: MIT + +#pragma once + +#include "geometry.hpp" +#include "ikineticfluidcoupling.hpp" +#include "itimesolver_hybrid.hpp" + +class IQNSolver; +class IBoltzmannSolver; +class IFluidTransportSolver; +class IKineticFluidCoupling; + +/** + * @brief A class that solves a Boltzmann-Poisson system of equations coupled to a fluid particles model using a predictor-corrector scheme. + * + * A class that solves a Boltzmann-Poisson system with + * a predictor corrector scheme. This scheme consists in + * estimating the electric potential after a time interval + * of a half-timestep. This potential is then used to compute + * the value of the distribution function at time t+dt, and the + * value of the fluid moments for the fluid species. + * The fluid moments value is computed first without the source term S_n,N(x) via the fluid_solver. + * Then, a coupling between the distribution function and the fluid moments is computed with the kinetic_fluid_coupling function. + * dt is the timestep of the simulation. + */ +class PredCorrHybrid : public ITimeSolverHybrid +{ +private: + IBoltzmannSolver const& m_boltzmann_solver; + + IFluidTransportSolver const& m_fluid_solver; + + IQNSolver const& m_poisson_solver; + + IKineticFluidCoupling const& m_kinetic_fluid_coupling; + +public: + /** + * @brief Creates an instance of the predictor-corrector class. + * @param[in] boltzmann_solver A solver for a Boltzmann equation. + * @param[in] fluid_solver A solver for a fluid model. + * @param[in] poisson_solver A solver for a Quasi-Neutrality equation. + * @param[in] kinetic_fluid_coupling A solver of the neutral source term in both the Boltzmann and fluid equations. + */ + PredCorrHybrid( + IBoltzmannSolver const& boltzmann_solver, + IFluidTransportSolver const& fluid_solver, + IQNSolver const& poisson_solver, + IKineticFluidCoupling const& kinetic_fluid_coupling); + + ~PredCorrHybrid() override = default; + + /** + * @brief Solves the Boltzmann-Poisson-fluid system. + * @param[in, out] allfdistribu On input: the initial value of the distribution function. + * On output: the value of the distribution function after solving + * the Boltzmann-Poisson-fluid system a given number of iterations. + ** @param[in, out] fluid_moments On input: a field referencing the fluid species. + * On output: the state of the fluid species after solving + * the Boltzmann-Poisson-fluid system a given number of iterations. + * @param[in] time_start The physical time at the start of the simulation. + * @param[in] dt The timestep. + * @param[in] steps The number of iterations to be performed by the predictor-corrector. + * @return The distribution function after solving the system. + */ + DFieldSpXVx operator()( + DFieldSpXVx allfdistribu, + DFieldSpMomX fluid_moments, + double time_start, + double dt, + int steps = 1) const override; +}; diff --git a/tests/geometryXVx/CMakeLists.txt b/tests/geometryXVx/CMakeLists.txt index c5167da9a..a88fc112a 100644 --- a/tests/geometryXVx/CMakeLists.txt +++ b/tests/geometryXVx/CMakeLists.txt @@ -27,6 +27,8 @@ target_link_libraries(unit_tests_${GEOMETRY_VARIANT} paraconf::paraconf gslx::advection gslx::boltzmann_${GEOMETRY_VARIANT} + gslx::fluidinitialization_${GEOMETRY_VARIANT} + gslx::fluidsolver_${GEOMETRY_VARIANT} gslx::moments gslx::poisson_${GEOMETRY_VARIANT} gslx::quadrature @@ -97,4 +99,8 @@ endif() add_subdirectory(bump_on_tail) +add_subdirectory(geometryMX) + add_subdirectory(landau) + +add_subdirectory(sheath) diff --git a/tests/geometryXVx/geometryMX/CMakeLists.txt b/tests/geometryXVx/geometryMX/CMakeLists.txt new file mode 100644 index 000000000..d1f62647f --- /dev/null +++ b/tests/geometryXVx/geometryMX/CMakeLists.txt @@ -0,0 +1,43 @@ +# SPDX-License-Identifier: MIT + + +include(GoogleTest) + +set(BASIC_GEOMETRY_XVx_VARIANTS_LIST xperiod_vx xnonperiod_vx) + +foreach(GEOMETRY_VARIANT IN LISTS BASIC_GEOMETRY_XVx_VARIANTS_LIST) + +add_executable(unit_tests_geometryMX_${GEOMETRY_VARIANT} + ../../main.cpp + fluidspecies.cpp + moments.cpp + predcorr_hybrid.cpp + diffusiveneutrals.cpp + ratecoefficients.cpp + kineticfluidcoupling.cpp +) + +target_link_libraries(unit_tests_geometryMX_${GEOMETRY_VARIANT} + PUBLIC + GTest::gtest + GTest::gmock + gslx::advection + gslx::boltzmann_${GEOMETRY_VARIANT} + gslx::fluidinitialization_${GEOMETRY_VARIANT} + gslx::fluidsolver_${GEOMETRY_VARIANT} + gslx::moments + gslx::poisson_${GEOMETRY_VARIANT} + gslx::quadrature + gslx::speciesinfo + gslx::time_integration_${GEOMETRY_VARIANT} + gslx::time_integration_hybrid_${GEOMETRY_VARIANT} + gslx::utils_${GEOMETRY_VARIANT} +) + +gtest_discover_tests(unit_tests_geometryMX_${GEOMETRY_VARIANT} + TEST_SUFFIX "_${GEOMETRY_VARIANT}" + PROPERTIES TIMEOUT 10 + DISCOVERY_MODE PRE_TEST +) + +endforeach() diff --git a/tests/geometryXVx/geometryMX/diffusiveneutrals.cpp b/tests/geometryXVx/geometryMX/diffusiveneutrals.cpp new file mode 100644 index 000000000..2d356b764 --- /dev/null +++ b/tests/geometryXVx/geometryMX/diffusiveneutrals.cpp @@ -0,0 +1,215 @@ +// SPDX-License-Identifier: MIT +#include + +#include +#include + +#include +#include + +#include "constantfluidinitialization.hpp" +#include "constantrate.hpp" +#include "ddc_alias_inline_functions.hpp" +#include "diffusiveneutralsolver.hpp" +#include "geometry.hpp" +#include "maxwellianequilibrium.hpp" +#include "quadrature.hpp" +#include "species_info.hpp" +#include "trapezoid_quadrature.hpp" + +/** + * This test initializes a neutral density with an exponential spatial variation + * and constant quantities for the kinetic species densities, temperature, etc. + * Then the time derivative of the diffusive neutral model is computed using the solver, + * and analytically. The two expressions for the derivative are compared and the relative + * difference between the two is checked to be within a percent. +*/ +TEST(GeometryMX, DiffusiveNeutralsDerivative) +{ + CoordX const x_min(0.0); + CoordX const x_max(10); + IdxStepX const x_size(512); + + CoordVx const vx_min(-8); + CoordVx const vx_max(8); + IdxStepVx const vx_size(50); + + // Creating mesh & supports + ddc::init_discrete_space(x_min, x_max, x_size); + + ddc::init_discrete_space(vx_min, vx_max, vx_size); + + ddc::init_discrete_space(SplineInterpPointsX::get_sampling()); + ddc::init_discrete_space(SplineInterpPointsVx::get_sampling()); + + IdxRangeX meshX(SplineInterpPointsX::get_domain()); + IdxRangeVx meshVx(SplineInterpPointsVx::get_domain()); + IdxRangeXVx meshXVx(meshX, meshVx); + + SplineXBuilder const builder_x(meshXVx); + SplineVxBuilder const builder_vx(meshXVx); + + // Kinetic species index range initialization + IdxStepSp const nb_kinspecies(2); + IdxRangeSp const idx_range_kinsp(IdxSp(0), nb_kinspecies); + + IdxSp const my_iion = idx_range_kinsp.front(); + IdxSp const my_ielec = idx_range_kinsp.back(); + + host_t kinetic_charges(idx_range_kinsp); + kinetic_charges(my_ielec) = -1.; + kinetic_charges(my_iion) = 1.; + + host_t kinetic_masses(idx_range_kinsp); + double const mass_ion(400.), mass_elec(1.); + kinetic_masses(my_ielec) = mass_elec; + kinetic_masses(my_iion) = mass_ion; + + // Neutral species index range initialization + IdxStepSp const nb_fluidspecies(1); + IdxRangeSp const idx_range_fluidsp(IdxSp(idx_range_kinsp.back() + 1), nb_fluidspecies); + IdxSp const my_ifluid = idx_range_fluidsp.front(); + + // neutrals charge is zero + host_t fluid_charges(idx_range_fluidsp); + ddc::parallel_fill(fluid_charges, 0.); + + host_t fluid_masses(idx_range_fluidsp); + double const neutral_mass(1.); + fluid_masses(my_ifluid) = neutral_mass; + + // Create the index range of kinetic species + fluid species + IdxRangeSp const idx_range_allsp(IdxSp(0), nb_kinspecies + nb_fluidspecies); + + // Create a Field that contains charges of all species + host_t charges(idx_range_allsp); + + // fill the Field with charges of kinetic species + for (IdxSp isp : idx_range_kinsp) { + charges(isp) = kinetic_charges(isp); + } + + // fill the Field with charges of fluid species + for (IdxSp isp : idx_range_fluidsp) { + charges(isp) = fluid_charges(isp); + } + + // Create a Field that contains masses of kinetic and fluid species + host_t masses(idx_range_allsp); + + // fill the Field with masses of kinetic species + for (IdxSp isp : idx_range_kinsp) { + masses(isp) = kinetic_masses(isp); + } + + // fill the Field with masses of fluid species + for (IdxSp isp : idx_range_fluidsp) { + masses(isp) = fluid_masses(isp); + } + + ddc::init_discrete_space(std::move(charges), std::move(masses)); + + // Moments index range initialization + IdxStepMom const nb_fluid_moments(1); + IdxRangeMom const meshM(IdxMom(0), nb_fluid_moments); + ddc::init_discrete_space(); + + // Neutral species initialization + double const charge_exchange_val(0.5); + double const ionization_val(1.); + double const recombination_val(2.); + double const normalization_coeff(1.); + +#ifdef PERIODIC_RDIMX + ddc::PeriodicExtrapolationRule bv_x_min; + ddc::PeriodicExtrapolationRule bv_x_max; +#else + ddc::ConstantExtrapolationRule bv_x_min(x_min); + ddc::ConstantExtrapolationRule bv_x_max(x_max); +#endif + + ConstantRate charge_exchange(charge_exchange_val); + ConstantRate ionization(ionization_val); + ConstantRate recombination(recombination_val); + + SplineXBuilder_1d const spline_x_builder_neutrals(meshX); + SplineXEvaluator_1d const spline_x_evaluator_neutrals(bv_x_min, bv_x_max); + + DFieldMemVx quadrature_coeffs_alloc( + trapezoid_quadrature_coefficients(meshVx)); + DFieldVx const quadrature_coeffs = get_field(quadrature_coeffs_alloc); + + DiffusiveNeutralSolver const neutralsolver( + charge_exchange, + ionization, + recombination, + normalization_coeff, + spline_x_builder_neutrals, + spline_x_evaluator_neutrals, + quadrature_coeffs); + + host_t neutrals_init_host(IdxRangeSpMomX(idx_range_fluidsp, meshM, meshX)); + ddc::for_each(get_idx_range(neutrals_init_host), [&](IdxSpMomX const ispmx) { + CoordX coordx(ddc::coordinate(ddc::select(ispmx))); + double const lx_2((x_max + x_min) / 2.); + neutrals_init_host(ispmx) = std::exp(-0.5 * (coordx - lx_2) * (coordx - lx_2)); + }); + + DFieldMemSpMomX neutrals_alloc(get_idx_range(neutrals_init_host)); + DFieldSpMomX neutrals = get_field(neutrals_alloc); + ddc::parallel_deepcopy(neutrals, neutrals_init_host); + + DFieldMemSpMomX derivative_alloc(get_idx_range(neutrals)); + DFieldSpMomX derivative = get_field(derivative_alloc); + + DFieldMemSpX kinsp_density_alloc(IdxRangeSpX(idx_range_kinsp, meshX)); + DFieldMemSpX kinsp_velocity_alloc(IdxRangeSpX(idx_range_kinsp, meshX)); + DFieldMemSpX kinsp_temperature_alloc(IdxRangeSpX(idx_range_kinsp, meshX)); + + DFieldSpX kinsp_density = get_field(kinsp_density_alloc); + DFieldSpX kinsp_velocity = get_field(kinsp_velocity_alloc); + DFieldSpX kinsp_temperature = get_field(kinsp_temperature_alloc); + + double const kinsp_density_eq(1.); + double const kinsp_velocity_eq(0.5); + double const kinsp_temperature_eq(1.); + ddc::parallel_fill(kinsp_density, kinsp_density_eq); + ddc::parallel_fill(kinsp_velocity, kinsp_velocity_eq); + ddc::parallel_fill(kinsp_temperature, kinsp_temperature_eq); + + neutralsolver.get_derivative( + derivative, + neutrals, + get_const_field(kinsp_density), + get_const_field(kinsp_velocity), + get_const_field(kinsp_temperature)); + + auto derivative_host = ddc::create_mirror_view_and_copy(derivative); + + double error_l1(0); + double max_derivative(0); + ddc::for_each(get_idx_range(neutrals), [&](IdxSpMomX const ispmx) { + double const neutral_val(neutrals_init_host(ispmx)); + + double const lx_2((x_max + x_min) / 2.); + CoordX coordx(ddc::coordinate(ddc::select(ispmx))); + double const neutral_val_deriv((lx_2 - coordx) * neutral_val); + double const neutral_val_deriv2(neutral_val * ((lx_2 - coordx) * (lx_2 - coordx) - 1.)); + + double const mass_ratio(mass(my_ielec) / mass(my_iion)); + + double const advec_term( + std::sqrt(mass_ratio) * kinsp_velocity_eq * charge_exchange_val + / (charge_exchange_val + ionization_val)); + double const diffusive_term( + normalization_coeff * kinsp_temperature_eq + / (neutral_mass * kinsp_density_eq * (charge_exchange_val + ionization_val))); + double const derivative_pred( + -advec_term * neutral_val_deriv + diffusive_term * neutral_val_deriv2); + + error_l1 += abs(derivative_pred - derivative_host(ispmx)); + max_derivative = abs(derivative_pred) > max_derivative ? derivative_pred : max_derivative; + }); + + EXPECT_LE(error_l1 / max_derivative, 0.01); +} diff --git a/tests/geometryXVx/geometryMX/fluidspecies.cpp b/tests/geometryXVx/geometryMX/fluidspecies.cpp new file mode 100644 index 000000000..594f8c81e --- /dev/null +++ b/tests/geometryXVx/geometryMX/fluidspecies.cpp @@ -0,0 +1,212 @@ +// SPDX-License-Identifier: MIT + +#include + +#include + +#include +#include + +#include + +#include "constantfluidinitialization.hpp" +#include "geometry.hpp" +#include "species_info.hpp" + +/** + * This test initializes a discrete space for kinetic species + * and fluid species, with corresponding masses and charges. + * The test checks if the masses() and charges() attributes + * of the discrete space correspond to the masses and charges + * attributes of the fluid and kinetic species. + */ +TEST(GeometryXM, KineticFluidSpecies) +{ + CoordX const x_min(0.0); + CoordX const x_max(1.0); + IdxStepX const x_size(50); + + // Creating mesh & supports + ddc::init_discrete_space(x_min, x_max, x_size); + ddc::init_discrete_space(SplineInterpPointsX::get_sampling()); + + IdxRangeX meshX(SplineInterpPointsX::get_domain()); + SplineXBuilder_1d const builder_x(meshX); + + // Kinetic species index range initialization + IdxStepSp const nb_kinspecies(2); + IdxRangeSp const idx_range_kinsp(IdxSp(0), nb_kinspecies); + + IdxSp const my_iion = idx_range_kinsp.front(); + IdxSp const my_ielec = idx_range_kinsp.back(); + + host_t kinetic_charges(idx_range_kinsp); + kinetic_charges(my_ielec) = -1.; + kinetic_charges(my_iion) = 1.; + + host_t kinetic_masses(idx_range_kinsp); + double const mass_ion(400.), mass_elec(1.); + kinetic_masses(my_ielec) = mass_elec; + kinetic_masses(my_iion) = mass_ion; + + // Fluid species index range initialization + IdxStepSp const nb_fluidspecies(2); + IdxRangeSp const idx_range_fluidsp(IdxSp(idx_range_kinsp.back() + 1), nb_fluidspecies); + + host_t fluid_charges(idx_range_fluidsp); + fluid_charges(idx_range_fluidsp.front()) = 1.; + fluid_charges(idx_range_fluidsp.back()) = -1.; + + host_t fluid_masses(idx_range_fluidsp); + fluid_masses(idx_range_fluidsp.front()) = 5.; + fluid_masses(idx_range_fluidsp.back()) = 8.; + + // Create the index range of kinetic species + fluid species + IdxRangeSp const idx_range_allsp(IdxSp(0), nb_kinspecies + nb_fluidspecies); + + // Create a Field that contains charges of all species + host_t charges(idx_range_allsp); + + // fill the Field with charges of kinetic species + for (IdxSp isp : idx_range_kinsp) { + charges(isp) = kinetic_charges(isp); + } + + // fill the Field with charges of fluid species + for (IdxSp isp : idx_range_fluidsp) { + charges(isp) = fluid_charges(isp); + } + + // Create a Field that contains masses of kinetic and fluid species + host_t masses(idx_range_allsp); + + // fill the Field with masses of kinetic species + for (IdxSp isp : idx_range_kinsp) { + masses(isp) = kinetic_masses(isp); + } + + // fill the Field with masses of fluid species + for (IdxSp isp : idx_range_fluidsp) { + masses(isp) = fluid_masses(isp); + } + + ddc::init_discrete_space(std::move(charges), std::move(masses)); + + ddc::for_each(idx_range_allsp, [&](IdxSp const isp) { + if (isp.uid() < nb_kinspecies) { + EXPECT_EQ(ddc::discrete_space().charges()(isp), kinetic_charges(isp)); + EXPECT_EQ(ddc::discrete_space().masses()(isp), kinetic_masses(isp)); + + } else if (nb_kinspecies + 1 <= isp.uid() && isp.uid() < nb_kinspecies + nb_fluidspecies) { + EXPECT_EQ(ddc::discrete_space().charges()(isp), fluid_charges(isp)); + EXPECT_EQ(ddc::discrete_space().masses()(isp), fluid_masses(isp)); + } + }); +} + +/** + * Same test as above with an adiabatic species + * on top of the fluid and kinetic species. + */ +TEST(GeometryXM, KineticFluidAdiabaticSpecies) +{ + CoordX const x_min(0.0); + CoordX const x_max(1.0); + IdxStepX const x_size(50); + + // Creating mesh & supports + ddc::init_discrete_space(x_min, x_max, x_size); + ddc::init_discrete_space(SplineInterpPointsX::get_sampling()); + + IdxRangeX meshX(SplineInterpPointsX::get_domain()); + SplineXBuilder_1d const builder_x(meshX); + + // Kinetic species index range initialization + IdxStepSp const nb_kinspecies(2); + IdxRangeSp const idx_range_kinsp(IdxSp(0), nb_kinspecies); + + IdxSp const my_iion = idx_range_kinsp.front(); + IdxSp const my_ielec = idx_range_kinsp.back(); + + host_t kinetic_charges(idx_range_kinsp); + kinetic_charges(my_ielec) = -1.; + kinetic_charges(my_iion) = 1.; + + host_t kinetic_masses(idx_range_kinsp); + double const mass_ion(400.), mass_elec(1.); + kinetic_masses(my_ielec) = mass_elec; + kinetic_masses(my_iion) = mass_ion; + + // adiabatic species initialization + int nb_ion_adiabspecies = 1; + + // Fluid species index range initialization + IdxStepSp const nb_fluidspecies(2); + IdxRangeSp const idx_range_fluidsp(IdxSp(idx_range_kinsp.back() + 1), nb_fluidspecies); + + host_t fluid_charges(idx_range_fluidsp); + fluid_charges(idx_range_fluidsp.front()) = 1.; + fluid_charges(idx_range_fluidsp.back()) = -1.; + + host_t fluid_masses(idx_range_fluidsp); + fluid_masses(idx_range_fluidsp.front()) = 5.; + fluid_masses(idx_range_fluidsp.back()) = 8.; + + // Create the index range of all species including kinetic species + fluid species + adiabatic species (if existing) + // adiabatic species are placed at the back of the index range + IdxRangeSp const + idx_range_allsp(IdxSp(0), nb_kinspecies + nb_fluidspecies + nb_ion_adiabspecies); + + // Create a Field that contains charges of all species + host_t charges(idx_range_allsp); + + // fill the Field with charges of kinetic species + for (IdxSp isp : idx_range_kinsp) { + charges(isp) = kinetic_charges(isp); + } + + // fill the Field with charges of fluid species + for (IdxSp isp : idx_range_fluidsp) { + charges(isp) = fluid_charges(isp); + } + + // fill the Field with charges of adiabatic species + double const charge_adiabspecies(3.); + charges(idx_range_allsp.back()) = nb_ion_adiabspecies * charge_adiabspecies; + + // Create the index range of kinetic and fluid species + IdxRangeSp const idx_range_kinfluidsp(IdxSp(0), nb_kinspecies + nb_fluidspecies); + + // Create a Field that contains masses of kinetic and fluid species (adiabatic species do not have a mass) + host_t masses(idx_range_kinfluidsp); + + // fill the Field with masses of kinetic species + for (IdxSp isp : idx_range_kinsp) { + masses(isp) = kinetic_masses(isp); + } + + // fill the Field with masses of fluid species + for (IdxSp isp : idx_range_fluidsp) { + masses(isp) = fluid_masses(isp); + } + ddc::init_discrete_space(std::move(charges), std::move(masses)); + + /** + * checks that the masses and charges of idx_range_allsp are well-ordered: + * kinetic species first, then fluid species, then adiabatic species. + */ + ddc::for_each(idx_range_allsp, [&](IdxSp const isp) { + if (isp.uid() < nb_kinspecies) { + EXPECT_EQ(ddc::discrete_space().charges()(isp), kinetic_charges(isp)); + EXPECT_EQ(ddc::discrete_space().masses()(isp), kinetic_masses(isp)); + + } else if (nb_kinspecies <= isp.uid() && isp.uid() < nb_kinspecies + nb_fluidspecies) { + EXPECT_EQ(ddc::discrete_space().charges()(isp), fluid_charges(isp)); + EXPECT_EQ(ddc::discrete_space().masses()(isp), fluid_masses(isp)); + + } else { + EXPECT_EQ(isp, idx_range_allsp.back()); + EXPECT_EQ(ddc::discrete_space().charges()(isp), charge_adiabspecies); + } + }); +} diff --git a/tests/geometryXVx/geometryMX/kineticfluidcoupling.cpp b/tests/geometryXVx/geometryMX/kineticfluidcoupling.cpp new file mode 100644 index 000000000..7fd72e076 --- /dev/null +++ b/tests/geometryXVx/geometryMX/kineticfluidcoupling.cpp @@ -0,0 +1,305 @@ +// SPDX-License-Identifier: MIT +#include + +#include +#include + +#include +#include + +#include + +#include "Lagrange_interpolator.hpp" +#include "bsl_advection_vx.hpp" +#include "bsl_advection_x.hpp" +#include "charge_exchange.hpp" +#include "chargedensitycalculator.hpp" +#include "constantfluidinitialization.hpp" +#include "ddc_alias_inline_functions.hpp" +#include "diffusiveneutralsolver.hpp" +#include "fem_1d_poisson_solver.hpp" +#include "fft_poisson_solver.hpp" +#include "geometry.hpp" +#include "ionization.hpp" +#include "irighthandside.hpp" +#include "kinetic_fluid_coupling_source.hpp" +#include "maxwellianequilibrium.hpp" +#include "neumann_spline_quadrature.hpp" +#include "predcorr.hpp" +#include "predcorr_hybrid.hpp" +#include "qnsolver.hpp" +#include "quadrature.hpp" +#include "recombination.hpp" +#include "singlemodeperturbinitialization.hpp" +#include "species_info.hpp" +#include "spline_interpolator.hpp" +#include "splitrighthandsidesolver.hpp" +#include "splitvlasovsolver.hpp" +#include "trapezoid_quadrature.hpp" + +/** + * This test initializes the fluid species with constant reaction rates for ionization and recombination. + * Then, using the analytical solution for this scenario where T is cte. we compare it to the solver. + */ +static void TestKineticFluidCoupling() +{ + CoordX const x_min(0.0); + CoordX const x_max(1.0); + IdxStepX const x_ncells(10); + + CoordVx const vx_min(-8); + CoordVx const vx_max(8); + IdxStepVx const vx_ncells(20); + + PC_tree_t conf_pdi = PC_parse_string(""); + PDI_init(conf_pdi); + + // Creating mesh & supports + ddc::init_discrete_space(x_min, x_max, x_ncells); + + ddc::init_discrete_space(vx_min, vx_max, vx_ncells); + + ddc::init_discrete_space(SplineInterpPointsX::get_sampling()); + ddc::init_discrete_space(SplineInterpPointsVx::get_sampling()); + + IdxRangeX meshX(SplineInterpPointsX::get_domain()); + IdxRangeVx meshVx(SplineInterpPointsVx::get_domain()); + IdxRangeXVx meshXVx(meshX, meshVx); + + SplineXBuilder const builder_x(meshXVx); +#ifndef PERIODIC_RDIMX + SplineXBuilder_1d const builder_x_poisson(meshX); +#endif + SplineVxBuilder const builder_vx(meshXVx); + SplineVxBuilder_1d const builder_vx_poisson(meshVx); + + // Kinetic species index range initialization + IdxStepSp const nb_kinspecies(2); + IdxRangeSp const idx_range_kinsp(IdxSp(0), nb_kinspecies); + + IdxSp const iion = idx_range_kinsp.front(); + IdxSp const ielec = idx_range_kinsp.back(); + + host_t> kinetic_charges(idx_range_kinsp); + kinetic_charges(ielec) = -1; + kinetic_charges(iion) = 1; + + host_t kinetic_masses(idx_range_kinsp); + double const mass_ion(400), mass_elec(1); + kinetic_masses(ielec) = mass_elec; + kinetic_masses(iion) = mass_ion; + + // Fluid species index range initialization + IdxStepSp const nb_fluidspecies(1); + IdxRangeSp const idx_range_fluidsp(IdxSp(idx_range_kinsp.back() + 1), nb_fluidspecies); + + // Fluid charges + host_t fluid_charges(idx_range_fluidsp); + ddc::parallel_fill(fluid_charges, 0.); + + host_t fluid_masses(idx_range_fluidsp); + ddc::parallel_fill(fluid_masses, mass_ion); + + // Create the index range of kinetic species + fluid species + IdxRangeSp const idx_range_allsp(IdxSp(0), nb_kinspecies + nb_fluidspecies); + + // Create a Field that contains charges of all species + host_t charges(idx_range_allsp); + + // fill the Field with charges of kinetic species + for (IdxSp isp : idx_range_kinsp) { + charges(isp) = kinetic_charges(isp); + } + + // fill the Field with charges of fluid species + for (IdxSp isp : idx_range_fluidsp) { + charges(isp) = fluid_charges(isp); + } + + // Create a Field that contains masses of kinetic and fluid species + host_t masses(idx_range_allsp); + + // fill the Field with masses of kinetic species + for (IdxSp isp : idx_range_kinsp) { + masses(isp) = kinetic_masses(isp); + } + + // fill the Field with masses of fluid species + for (IdxSp isp : idx_range_fluidsp) { + masses(isp) = fluid_masses(isp); + } + + ddc::init_discrete_space(std::move(charges), std::move(masses)); + + // Initialization of kinetic species distribution function + DFieldMemSpXVx allfdistribu_alloc(IdxRangeSpXVx(idx_range_kinsp, meshX, meshVx)); + DFieldSpXVx allfdistribu = get_field(allfdistribu_alloc); + + host_t kinsp_density_eq(idx_range_kinsp); + host_t kinsp_velocity_eq(idx_range_kinsp); + host_t kinsp_temperature_eq(idx_range_kinsp); + + ddc::parallel_fill(kinsp_density_eq, 1.); + ddc::parallel_fill(kinsp_velocity_eq, 0.); + ddc::parallel_fill(kinsp_temperature_eq, 1.); + + DFieldMemSpVx allfequilibrium_alloc(IdxRangeSpVx(idx_range_kinsp, meshVx)); + DFieldSpVx allfequilibrium = get_field(allfequilibrium_alloc); + MaxwellianEquilibrium const init_fequilibrium( + std::move(kinsp_density_eq), + std::move(kinsp_temperature_eq), + std::move(kinsp_velocity_eq)); + init_fequilibrium(allfequilibrium); + + host_t init_perturb_mode(idx_range_kinsp); + host_t init_perturb_amplitude(idx_range_kinsp); + ddc::parallel_fill(init_perturb_mode, 1); + ddc::parallel_fill(init_perturb_amplitude, 0.0); + + SingleModePerturbInitialization const + init(allfequilibrium, std::move(init_perturb_mode), std::move(init_perturb_amplitude)); + init(allfdistribu); + + // Moments index range initialization + IdxStepMom const nb_fluid_moments(1); + IdxRangeMom const meshM(IdxMom(0), nb_fluid_moments); + ddc::init_discrete_space(); + + // Initialization of fluid species moments + DFieldMemSpMomX fluid_moments_alloc(IdxRangeSpMomX(idx_range_fluidsp, meshM, meshX)); + DFieldSpMomX fluid_moments = get_field(fluid_moments_alloc); + + host_t moments_init(IdxRangeSpMom(idx_range_fluidsp, meshM)); + ddc::parallel_fill(moments_init, 0.); + ConstantFluidInitialization fluid_init(moments_init); + fluid_init(fluid_moments); + +#ifdef PERIODIC_RDIMX + ddc::PeriodicExtrapolationRule bv_x_min; + ddc::PeriodicExtrapolationRule bv_x_max; +#else + ddc::ConstantExtrapolationRule bv_x_min(x_min); + ddc::ConstantExtrapolationRule bv_x_max(x_max); +#endif + + // Creating operators + SplineXEvaluator const spline_x_evaluator(bv_x_min, bv_x_max); +#ifndef PERIODIC_RDIMX + SplineXEvaluator_1d const spline_x_evaluator_poisson(bv_x_min, bv_x_max); +#endif + PreallocatableSplineInterpolator const spline_x_interpolator(builder_x, spline_x_evaluator); + + IdxStepVx static constexpr gwvx {0}; + LagrangeInterpolator const + lagrange_vx_non_preallocatable_interpolator(3, gwvx); + PreallocatableLagrangeInterpolator< + GridVx, + BCond::DIRICHLET, + BCond::DIRICHLET, + GridX, + GridVx> const lagrange_vx_interpolator(lagrange_vx_non_preallocatable_interpolator); + + BslAdvectionSpatial const advection_x(spline_x_interpolator); + BslAdvectionVelocity const advection_vx(lagrange_vx_interpolator); + + SplitVlasovSolver const vlasov(advection_x, advection_vx); + + DFieldMemVx const quadrature_coeffs(neumann_spline_quadrature_coefficients< + Kokkos::DefaultExecutionSpace>(meshVx, builder_vx_poisson)); + + ChargeDensityCalculator rhs(get_const_field(quadrature_coeffs)); +#ifdef PERIODIC_RDIMX + FFTPoissonSolver poisson_solver(meshX); +#else + FEM1DPoissonSolver const poisson_solver(builder_x_poisson, spline_x_evaluator_poisson); +#endif + QNSolver const poisson(poisson_solver, rhs); + + double const normalization_coeff(0.01); + double const k_0(1.e-3); + + ChargeExchangeRate charge_exchange(k_0); + IonizationRate ionization(k_0); + RecombinationRate recombination(k_0); + + SplineXBuilder_1d const spline_x_builder_neutrals(meshX); + SplineXEvaluator_1d const spline_x_evaluator_neutrals(bv_x_min, bv_x_max); + + DFieldMemVx const quadrature_coeffs_neutrals( + trapezoid_quadrature_coefficients(meshVx)); + + + DiffusiveNeutralSolver const fluidsolver( + charge_exchange, + ionization, + recombination, + normalization_coeff, + spline_x_builder_neutrals, + spline_x_evaluator_neutrals, + get_const_field(quadrature_coeffs_neutrals)); + + // kinetic fluid coupling term + KineticFluidCouplingSource const kineticfluidcoupling( + 1., + 0., + 0., + ionization, + recombination, + normalization_coeff, + quadrature_coeffs); + + double const time_start(0.); + int const nb_iter(20); + double const deltat(0.1); + + PredCorrHybrid const predcorr_hybrid(vlasov, fluidsolver, poisson, kineticfluidcoupling); + predcorr_hybrid(allfdistribu, fluid_moments, time_start, deltat, nb_iter); + + auto allfdistribu_host = ddc::create_mirror_view_and_copy(allfdistribu); + auto fluid_moments_host = ddc::create_mirror_view_and_copy(fluid_moments); + + // analytical solution + // we know the rate values for the initial conditions, we assume T=cte. so rates independent of time. + double const ionization_rate = 1.130359390036803 * k_0; + double const recombination_rate = 7.638123065868132e-06 * k_0; + + double const N = 1.; + double const alpha = -(N * ionization_rate) / normalization_coeff; + double const beta = -(ionization_rate + recombination_rate) / (2 * normalization_coeff); + double const C = (recombination_rate + ionization_rate) + / (2 * (0.0 * ionization_rate - 1.0 * recombination_rate)); + double const X_1 + = N * (recombination_rate - ionization_rate) / (recombination_rate + ionization_rate); + + DFieldMemSpMomX X_alloc(IdxRangeSpMomX(idx_range_fluidsp, meshM, meshX)); + DFieldSpMomX X = get_field(X_alloc); + DFieldMemSpMomX analytical_nN_alloc(IdxRangeSpMomX(idx_range_fluidsp, meshM, meshX)); + DFieldSpMomX analytical_nN = get_field(analytical_nN_alloc); + double const t_diag = nb_iter * deltat; + + ddc::parallel_for_each( + Kokkos::DefaultExecutionSpace(), + get_idx_range(X), + KOKKOS_LAMBDA(IdxSpMomX const ispmx) { + X(ispmx) = Kokkos::exp(alpha * t_diag) + * Kokkos:: + pow((beta / alpha) * Kokkos::expm1(alpha * t_diag) + C, + -1) + + X_1; + analytical_nN(ispmx) = (X(ispmx) + N) / 2.; + }); + + auto analytical_nN_host = ddc::create_mirror_view_and_copy(analytical_nN); + + ddc::for_each(get_idx_range(fluid_moments_host), [&](IdxSpMomX const ispmx) { + EXPECT_NEAR(analytical_nN_host(ispmx), fluid_moments_host(ispmx), 1.5e-8); + }); + + PC_tree_destroy(&conf_pdi); + PDI_finalize(); +} + +TEST(GeometryMX, KineticFluidCoupling) +{ + TestKineticFluidCoupling(); +} diff --git a/tests/geometryXVx/geometryMX/moments.cpp b/tests/geometryXVx/geometryMX/moments.cpp new file mode 100644 index 000000000..d9eb33297 --- /dev/null +++ b/tests/geometryXVx/geometryMX/moments.cpp @@ -0,0 +1,143 @@ +// SPDX-License-Identifier: MIT +#include + +#include + +#include +#include + +#include + +#include "constantfluidinitialization.hpp" +#include "ddc_alias_inline_functions.hpp" +#include "geometry.hpp" +#include "species_info.hpp" + +/** + * This test initializes a discrete space for moments (density, + * particle_flux, stress) and initializes a neutral species + * defined on the moment space and a spatial dimension with constant values + * for the density, particle flux and stress. The test checks if the + * initialization works properly. + */ +TEST(GeometryXM, MomentsInitialization) +{ + CoordX const x_min(0.0); + CoordX const x_max(1.0); + IdxStepX const x_size(50); + + // Creating mesh & supports + ddc::init_discrete_space(x_min, x_max, x_size); + ddc::init_discrete_space(SplineInterpPointsX::get_sampling()); + + IdxRangeX meshX(SplineInterpPointsX::get_domain()); + SplineXBuilder_1d const builder_x(meshX); + + // Kinetic species index range initialization + IdxStepSp const nb_kinspecies(2); + IdxRangeSp const idx_range_kinsp(IdxSp(0), nb_kinspecies); + + IdxSp const iion = idx_range_kinsp.front(); + IdxSp const ielec = idx_range_kinsp.back(); + + host_t kinetic_charges(idx_range_kinsp); + kinetic_charges(ielec) = -1.; + kinetic_charges(iion) = 1.; + + host_t kinetic_masses(idx_range_kinsp); + double const mass_ion(400.), mass_elec(1.); + kinetic_masses(ielec) = mass_elec; + kinetic_masses(iion) = mass_ion; + + // Neutral species index range initialization + IdxStepSp const nb_fluidspecies(1); + IdxRangeSp const idx_range_fluidsp(IdxSp(idx_range_kinsp.back() + 1), nb_fluidspecies); + IdxSp const ifluid = idx_range_fluidsp.front(); + + // neutrals charge is zero + host_t fluid_charges(idx_range_fluidsp); + ddc::parallel_fill(fluid_charges, 0.); + + host_t fluid_masses(idx_range_fluidsp); + fluid_masses(ifluid) = kinetic_masses(iion); + + // Create the index range of kinetic species + fluid species + IdxRangeSp const idx_range_allsp(IdxSp(0), nb_kinspecies + nb_fluidspecies); + + // Create a Field that contains charges of all species + host_t charges(idx_range_allsp); + + // fill the Field with charges of kinetic species + for (IdxSp isp : idx_range_kinsp) { + charges(isp) = kinetic_charges(isp); + } + + // fill the Field with charges of fluid species + for (IdxSp isp : idx_range_fluidsp) { + charges(isp) = fluid_charges(isp); + } + + // Create a Field that contains masses of kinetic and fluid species + host_t masses(idx_range_allsp); + + // fill the Field with masses of kinetic species + for (IdxSp isp : idx_range_kinsp) { + masses(isp) = kinetic_masses(isp); + } + + // fill the Field with masses of fluid species + for (IdxSp isp : idx_range_fluidsp) { + masses(isp) = fluid_masses(isp); + } + + ddc::init_discrete_space(std::move(charges), std::move(masses)); + + // Moments index range initialization + IdxStepMom const nb_fluid_moments(3); + IdxRangeMom const meshM(IdxMom(0), nb_fluid_moments); + ddc::init_discrete_space(); + + IdxMom idensity(0); + IdxMom iparticle_flux(1); + IdxMom istress(2); + + // Neutral species initialization + DFieldMemSpMomX neutrals_alloc(IdxRangeSpMomX(idx_range_fluidsp, meshM, meshX)); + DFieldSpMomX neutrals = get_field(neutrals_alloc); + + double const fluid_density_init(1.); + double const fluid_particle_flux_init(0.5); + double const fluid_stress_init(0.9); + + host_t moments_init_alloc(IdxRangeSpMom(idx_range_fluidsp, meshM)); + host_t moments_init = get_field(moments_init_alloc); + + moments_init(ifluid, idensity) = fluid_density_init; + moments_init(ifluid, iparticle_flux) = fluid_particle_flux_init; + moments_init(ifluid, istress) = fluid_stress_init; + + ConstantFluidInitialization fluid_init(moments_init); + fluid_init(neutrals); + + auto neutrals_host = ddc::create_mirror_view_and_copy(neutrals); + + double const tolerance(1.e-12); + ddc::for_each(get_idx_range(neutrals_host), [&](IdxSpX const ispx) { + IdxSp const isp(ddc::select(ispx)); + IdxX const ix(ddc::select(ispx)); + + // test for equality of density + IdxSpMomX const idensity_loc(isp, idensity, ix); + EXPECT_LE(std::fabs(neutrals_host(idensity_loc) - fluid_density_init), tolerance); + + // test for equality of particle_flux + IdxSpMomX const iparticle_flux_loc(isp, iparticle_flux, ix); + EXPECT_LE( + std::fabs(neutrals_host(iparticle_flux_loc) - fluid_particle_flux_init), + tolerance); + + // test for equality of stresses + IdxSpMomX const istress_loc(isp, istress, ix); + EXPECT_LE(std::fabs(neutrals_host(istress_loc) - fluid_stress_init), tolerance); + }); +} diff --git a/tests/geometryXVx/geometryMX/predcorr_hybrid.cpp b/tests/geometryXVx/geometryMX/predcorr_hybrid.cpp new file mode 100644 index 000000000..ecebcda30 --- /dev/null +++ b/tests/geometryXVx/geometryMX/predcorr_hybrid.cpp @@ -0,0 +1,275 @@ +// SPDX-License-Identifier: MIT +#include + +#include +#include + +#include +#include + +#include + +#include "Lagrange_interpolator.hpp" +#include "bsl_advection_vx.hpp" +#include "bsl_advection_x.hpp" +#include "chargedensitycalculator.hpp" +#include "constantfluidinitialization.hpp" +#include "constantrate.hpp" +#include "ddc_alias_inline_functions.hpp" +#include "fem_1d_poisson_solver.hpp" +#include "fft_poisson_solver.hpp" +#include "geometry.hpp" +#include "ikineticfluidcoupling.hpp" +#include "kinetic_fluid_coupling_source.hpp" +#include "maxwellianequilibrium.hpp" +#include "neumann_spline_quadrature.hpp" +#include "nullfluidsolver.hpp" +#include "predcorr.hpp" +#include "predcorr_hybrid.hpp" +#include "qnsolver.hpp" +#include "quadrature.hpp" +#include "singlemodeperturbinitialization.hpp" +#include "species_info.hpp" +#include "spline_interpolator.hpp" +#include "splitrighthandsidesolver.hpp" +#include "splitvlasovsolver.hpp" + +/** + * This test creates one instance of the PredCorr class, and one instance of the + * PredCorrFluid class. With the NullFluidSolver class, + * this test verifies that the distribution function is the same after applying the + * predictor corrector scheme to it, with and without the fluid species. + */ +TEST(GeometryXM, PredCorrHybrid) +{ + CoordX const x_min(0.0); + CoordX const x_max(1.0); + IdxStepX const x_ncells(50); + + CoordVx const vx_min(-8); + CoordVx const vx_max(8); + IdxStepVx const vx_ncells(50); + + PC_tree_t conf_pdi = PC_parse_string(""); + PDI_init(conf_pdi); + + // Creating mesh & supports + ddc::init_discrete_space(x_min, x_max, x_ncells); + + ddc::init_discrete_space(vx_min, vx_max, vx_ncells); + + ddc::init_discrete_space(SplineInterpPointsX::get_sampling()); + ddc::init_discrete_space(SplineInterpPointsVx::get_sampling()); + + IdxRangeX meshX(SplineInterpPointsX::get_domain()); + IdxRangeVx meshVx(SplineInterpPointsVx::get_domain()); + IdxRangeXVx meshXVx(meshX, meshVx); + + SplineXBuilder const builder_x(meshXVx); +#ifndef PERIODIC_RDIMX + SplineXBuilder_1d const builder_x_poisson(meshX); +#endif + SplineVxBuilder const builder_vx(meshXVx); + SplineVxBuilder_1d const builder_vx_poisson(meshVx); + + // Kinetic species index range initialization + IdxStepSp const nb_kinspecies(2); + IdxRangeSp const idx_range_kinsp(IdxSp(0), nb_kinspecies); + + IdxSp const iion = idx_range_kinsp.front(); + IdxSp const ielec = idx_range_kinsp.back(); + + host_t kinetic_charges(idx_range_kinsp); + kinetic_charges(ielec) = -1.; + kinetic_charges(iion) = 1.; + + host_t kinetic_masses(idx_range_kinsp); + double const mass_ion(400.), mass_elec(1.); + kinetic_masses(ielec) = mass_elec; + kinetic_masses(iion) = mass_ion; + + // Fluid species index range initialization + IdxStepSp const nb_fluidspecies(1); + IdxRangeSp const idx_range_fluidsp(IdxSp(idx_range_kinsp.back() + 1), nb_fluidspecies); + + // Fluid charges + host_t fluid_charges(idx_range_fluidsp); + ddc::parallel_fill(fluid_charges, 0.); + + host_t fluid_masses(idx_range_fluidsp); + ddc::parallel_fill(fluid_masses, mass_ion); + + // Create the index range of kinetic species + fluid species + IdxRangeSp const idx_range_allsp(IdxSp(0), nb_kinspecies + nb_fluidspecies); + + // Create a Field that contains charges of all species + host_t charges(idx_range_allsp); + + // fill the Field with charges of kinetic species + for (IdxSp isp : idx_range_kinsp) { + charges(isp) = kinetic_charges(isp); + } + + // fill the Field with charges of fluid species + for (IdxSp isp : idx_range_fluidsp) { + charges(isp) = fluid_charges(isp); + } + + // Create a Field that contains masses of kinetic and fluid species + host_t masses(idx_range_allsp); + + // fill the Field with masses of kinetic species + for (IdxSp isp : idx_range_kinsp) { + masses(isp) = kinetic_masses(isp); + } + + // fill the Field with masses of fluid species + for (IdxSp isp : idx_range_fluidsp) { + masses(isp) = fluid_masses(isp); + } + + ddc::init_discrete_space(std::move(charges), std::move(masses)); + + // Initialization of kinetic species distribution function + DFieldMemSpXVx allfdistribu_alloc(IdxRangeSpXVx(idx_range_kinsp, meshX, meshVx)); + DFieldSpXVx allfdistribu = get_field(allfdistribu_alloc); + + host_t kinsp_density_eq(idx_range_kinsp); + host_t kinsp_velocity_eq(idx_range_kinsp); + host_t kinsp_temperature_eq(idx_range_kinsp); + + ddc::parallel_fill(kinsp_density_eq, 1.); + ddc::parallel_fill(kinsp_velocity_eq, 0.); + ddc::parallel_fill(kinsp_temperature_eq, 1.); + + DFieldMemSpVx allfequilibrium_alloc(IdxRangeSpVx(idx_range_kinsp, meshVx)); + DFieldSpVx allfequilibrium = get_field(allfequilibrium_alloc); + MaxwellianEquilibrium const init_fequilibrium( + std::move(kinsp_density_eq), + std::move(kinsp_temperature_eq), + std::move(kinsp_velocity_eq)); + init_fequilibrium(allfequilibrium); + + host_t> init_perturb_mode(idx_range_kinsp); + ddc::parallel_fill(init_perturb_mode, 2); + host_t init_perturb_amplitude(idx_range_kinsp); + ddc::parallel_fill(init_perturb_amplitude, 0.1); + + SingleModePerturbInitialization const + init(allfequilibrium, std::move(init_perturb_mode), std::move(init_perturb_amplitude)); + init(allfdistribu); + + // Moments index range initialization + IdxStepMom const nb_fluid_moments(3); + IdxRangeMom const meshM(IdxMom(0), nb_fluid_moments); + ddc::init_discrete_space(); + + IdxMom idensity(0); + IdxMom iflux(1); + IdxMom istress(2); + + // Initialization of fluid species moments + DFieldMemSpMomX fluid_moments_alloc(IdxRangeSpMomX(idx_range_fluidsp, meshM, meshX)); + DFieldSpMomX fluid_moments = get_field(fluid_moments_alloc); + + host_t moments_init(IdxRangeSpMom(idx_range_fluidsp, meshM)); + ddc::parallel_fill(moments_init[idensity], 1.); + ddc::parallel_fill(moments_init[iflux], 0.); + ddc::parallel_fill(moments_init[istress], 1.); + + ConstantFluidInitialization fluid_init(moments_init); + fluid_init(fluid_moments); + +#ifdef PERIODIC_RDIMX + ddc::PeriodicExtrapolationRule bv_x_min; + ddc::PeriodicExtrapolationRule bv_x_max; +#else + ddc::ConstantExtrapolationRule bv_x_min(x_min); + ddc::ConstantExtrapolationRule bv_x_max(x_max); +#endif + + // Creating operators + SplineXEvaluator const spline_x_evaluator(bv_x_min, bv_x_max); +#ifndef PERIODIC_RDIMX + SplineXEvaluator_1d const spline_x_evaluator_poisson(bv_x_min, bv_x_max); +#endif + PreallocatableSplineInterpolator const spline_x_interpolator(builder_x, spline_x_evaluator); + + IdxStepVx static constexpr gwvx {0}; + LagrangeInterpolator const + lagrange_vx_non_preallocatable_interpolator(3, gwvx); + PreallocatableLagrangeInterpolator< + GridVx, + BCond::DIRICHLET, + BCond::DIRICHLET, + GridX, + GridVx> const lagrange_vx_interpolator(lagrange_vx_non_preallocatable_interpolator); + + BslAdvectionSpatial const advection_x(spline_x_interpolator); + BslAdvectionVelocity const advection_vx(lagrange_vx_interpolator); + + SplitVlasovSolver const vlasov(advection_x, advection_vx); + + DFieldMemVx const quadrature_coeffs = neumann_spline_quadrature_coefficients< + Kokkos::DefaultExecutionSpace>(meshVx, builder_vx_poisson); + + ChargeDensityCalculator rhs(get_const_field(quadrature_coeffs)); +#ifdef PERIODIC_RDIMX + FFTPoissonSolver poisson_solver(meshX); +#else + FEM1DPoissonSolver const poisson_solver(builder_x_poisson, spline_x_evaluator_poisson); +#endif + QNSolver const poisson(poisson_solver, rhs); + + ConstantRate const charge_exchange(0.0); + ConstantRate const ionization(0.0); + ConstantRate const recombination(0.0); + double const normalization_coeff(1.0); + + // kinetic fluid coupling term + KineticFluidCouplingSource const kineticfluidcoupling( + 1.0, + 0.0, + 0.0, + ionization, + recombination, + normalization_coeff, + quadrature_coeffs); + + // construction of predcorr without fluid species + PredCorr const predcorr(vlasov, poisson); + + // distribution function to be evolved by predcorr without fluid species + DFieldMemSpXVx allfdistribu_predcorr_alloc(get_idx_range(allfdistribu)); + DFieldSpXVx allfdistribu_predcorr = get_field(allfdistribu_predcorr_alloc); + ddc::parallel_deepcopy(allfdistribu_predcorr, allfdistribu); + + double const time_start(0.); + int const nb_iter(10); + double const deltat(0.1); + predcorr(allfdistribu_predcorr, time_start, deltat, nb_iter); + + // construction of predcorr with fluid species + NullFluidSolver const fluidsolver(idx_range_fluidsp); + PredCorrHybrid const predcorr_hybrid(vlasov, fluidsolver, poisson, kineticfluidcoupling); + predcorr_hybrid(allfdistribu, fluid_moments, time_start, deltat, nb_iter); + + auto allfdistribu_host = ddc::create_mirror_view_and_copy(allfdistribu); + + auto allfdistribu_predcorr_host = ddc::create_mirror_view_and_copy(allfdistribu_predcorr); + + /** + * Since the fluid model uses NullFluidSolver, + * the distribution function evolved with PredCorrFluid and PredCorr + * should be equal + */ + double const tolerance(1.e-12); + ddc::for_each(get_idx_range(allfdistribu), [&](IdxSpXVx const ispxvx) { + EXPECT_LE( + std::fabs(allfdistribu_host(ispxvx) - allfdistribu_predcorr_host(ispxvx)), + tolerance); + }); + + PC_tree_destroy(&conf_pdi); + PDI_finalize(); +} diff --git a/tests/geometryXVx/geometryMX/ratecoefficients.cpp b/tests/geometryXVx/geometryMX/ratecoefficients.cpp new file mode 100644 index 000000000..0a3b231f0 --- /dev/null +++ b/tests/geometryXVx/geometryMX/ratecoefficients.cpp @@ -0,0 +1,178 @@ +// SPDX-License-Identifier: MIT +#include + +#include +#include + +#include +#include + +#include + +#include "charge_exchange.hpp" +#include "constantfluidinitialization.hpp" +#include "ddc_alias_inline_functions.hpp" +#include "diffusiveneutralsolver.hpp" +#include "geometry.hpp" +#include "ionization.hpp" +#include "maxwellianequilibrium.hpp" +#include "quadrature.hpp" +#include "recombination.hpp" +#include "species_info.hpp" + + +/** + * This test initializes a neutral density with a flat spatial profile + * and constant quantities for the kinetic plasma species densities, temperature, etc. + * Then the time derivative of the diffusive neutral model is computed using the solver, + * and analytically. The two expressions for the derivative are compared and the relative + * difference between the two is checked to be within a percent. +*/ +static void TestDiffusiveNeutralsRateCoefficients() +{ + CoordX const x_min(0.0); + CoordX const x_max(10); + IdxStepX const x_size(512); + + CoordVx const vx_min(-8); + CoordVx const vx_max(8); + IdxStepVx const vx_size(50); + + PC_tree_t conf_pdi = PC_parse_string(""); + PDI_init(conf_pdi); + + // Creating mesh & supports + ddc::init_discrete_space(x_min, x_max, x_size); + + ddc::init_discrete_space(vx_min, vx_max, vx_size); + + ddc::init_discrete_space(SplineInterpPointsX::get_sampling()); + ddc::init_discrete_space(SplineInterpPointsVx::get_sampling()); + + IdxRangeX meshX(SplineInterpPointsX::get_domain()); + IdxRangeVx meshVx(SplineInterpPointsVx::get_domain()); + IdxRangeXVx meshXVx(meshX, meshVx); + + // Kinetic and neutral species index range initialization + IdxStepSp const nb_kinspecies(2); + IdxRangeSp const idx_range_kinsp(IdxSp(0), nb_kinspecies); + + IdxStepSp const nb_fluidspecies(1); + IdxRangeSp const idx_range_fluidsp(IdxSp(idx_range_kinsp.back() + 1), nb_fluidspecies); + + IdxRangeSp const idx_range_allsp(IdxSp(0), nb_kinspecies + nb_fluidspecies); + + host_t masses(idx_range_allsp); + host_t kinetic_masses = masses[idx_range_kinsp]; + host_t fluid_masses = masses[idx_range_fluidsp]; + + host_t charges(idx_range_allsp); + host_t kinetic_charges = charges[idx_range_kinsp]; + host_t fluid_charges = charges[idx_range_fluidsp]; + + IdxSp const my_iion = idx_range_kinsp.front(); + IdxSp const my_ielec = idx_range_kinsp.back(); + IdxSp const my_ifluid = idx_range_fluidsp.front(); + + kinetic_charges(my_ielec) = -1.; + kinetic_charges(my_iion) = 1.; + + double const mass_ion(400.), mass_elec(1.); + kinetic_masses(my_ielec) = mass_elec; + kinetic_masses(my_iion) = mass_ion; + + // neutrals charge is zero + fluid_charges(my_ifluid) = 0.; + + double const neutral_mass(1.); + fluid_masses(my_ifluid) = neutral_mass; + + ddc::init_discrete_space(std::move(charges), std::move(masses)); + + // Moments index range initialization + IdxStepMom const nb_fluid_moments(1); + IdxRangeMom const meshM(IdxMom(0), nb_fluid_moments); + ddc::init_discrete_space(); + + IdxRangeSpX idx_range_fluidspx = IdxRangeSpX(idx_range_fluidsp, meshX); + + ChargeExchangeRate charge_exchange(1.); + IonizationRate ionization(1.); + RecombinationRate recombination(1.); + + DFieldMemSpMomX neutrals_alloc(IdxRangeSpMomX(idx_range_fluidsp, meshM, meshX)); + DFieldSpMomX neutrals = get_field(neutrals_alloc); + + host_t moments_init(IdxRangeSpMom(idx_range_fluidsp, meshM)); + ddc::parallel_fill(moments_init, 1.); + ConstantFluidInitialization fluid_init(moments_init); + fluid_init(neutrals); + + DFieldMemSpMomX derivative_alloc(get_idx_range(neutrals)); + DFieldSpMomX derivative = get_field(derivative_alloc); + + DFieldMemSpX kinsp_density_alloc(IdxRangeSpX(idx_range_kinsp, meshX)); + DFieldMemSpX kinsp_velocity_alloc(IdxRangeSpX(idx_range_kinsp, meshX)); + DFieldMemSpX kinsp_temperature_alloc(IdxRangeSpX(idx_range_kinsp, meshX)); + + DFieldSpX kinsp_density = get_field(kinsp_density_alloc); + DFieldSpX kinsp_velocity = get_field(kinsp_velocity_alloc); + DFieldSpX kinsp_temperature = get_field(kinsp_temperature_alloc); + + double const kinsp_density_eq(1.); + double const kinsp_velocity_eq(0.0); + double const kinsp_temperature_eq(1.); + ddc::parallel_fill(kinsp_density, kinsp_density_eq); + ddc::parallel_fill(kinsp_velocity, kinsp_velocity_eq); + ddc::parallel_fill(kinsp_temperature, kinsp_temperature_eq); + + // building reaction rates + DFieldMemSpX charge_exchange_rate_alloc(idx_range_fluidspx); + DFieldMemSpX ionization_rate_alloc(idx_range_fluidspx); + DFieldMemSpX recombination_rate_alloc(idx_range_fluidspx); + + DFieldSpX charge_exchange_rate = get_field(charge_exchange_rate_alloc); + DFieldSpX ionization_rate = get_field(ionization_rate_alloc); + DFieldSpX recombination_rate = get_field(recombination_rate_alloc); + + charge_exchange(charge_exchange_rate, kinsp_density, kinsp_temperature); + ionization(ionization_rate, kinsp_density, kinsp_temperature); + recombination(recombination_rate, kinsp_density, kinsp_temperature); + + double mean_cx_rate = ddc::parallel_transform_reduce( + Kokkos::DefaultExecutionSpace(), + idx_range_fluidspx, + 0., + ddc::reducer::sum(), + charge_exchange_rate); + + double mean_i_rate = ddc::parallel_transform_reduce( + Kokkos::DefaultExecutionSpace(), + idx_range_fluidspx, + 0., + ddc::reducer::sum(), + ionization_rate); + + double mean_r_rate = ddc::parallel_transform_reduce( + Kokkos::DefaultExecutionSpace(), + idx_range_fluidspx, + 0., + ddc::reducer::sum(), + recombination_rate); + + mean_cx_rate /= meshX.size(); + mean_i_rate /= meshX.size(); + mean_r_rate /= meshX.size(); + + EXPECT_NEAR(mean_cx_rate, 1.783406341061044, 1e-13); + EXPECT_NEAR(mean_i_rate, 1.130359390036803, 1e-13); + EXPECT_NEAR(mean_r_rate, 7.638123065868132e-06, 1e-13); + + PC_tree_destroy(&conf_pdi); + PDI_finalize(); +} + +TEST(GeometryMX, NeutralsRateCoefficients) +{ + TestDiffusiveNeutralsRateCoefficients(); +} diff --git a/tests/geometryXVx/sheath/CMakeLists.txt b/tests/geometryXVx/sheath/CMakeLists.txt new file mode 100644 index 000000000..9b1935768 --- /dev/null +++ b/tests/geometryXVx/sheath/CMakeLists.txt @@ -0,0 +1,27 @@ +# SPDX-License-Identifier: MIT + +find_package(Python3 REQUIRED COMPONENTS Interpreter) + +if (${ACTIVATE_RESTART_TESTS}) + add_test(NAME TestSimulationSheathRestart_xperiod_vx + COMMAND bash "${CMAKE_CURRENT_SOURCE_DIR}/test_sheath_restart.sh" + "${PROJECT_SOURCE_DIR}" + "$" + "$" + "restart" + "${RELATIVE_RESTART_TOLERANCE}" + "${ABSOLUTE_RESTART_TOLERANCE}") + set_property(TEST TestSimulationSheathRestart_xperiod_vx PROPERTY TIMEOUT 200) + set_property(TEST TestSimulationSheathRestart_xperiod_vx PROPERTY COST 100) + + add_test(NAME TestSimulationSheathRestart_xperiod_vx_user_defined_grid + COMMAND bash "${CMAKE_CURRENT_SOURCE_DIR}/test_sheath_restart_user_defined_grid.sh" + "${PROJECT_SOURCE_DIR}" + "$" + "$" + "restart" + "${RELATIVE_RESTART_TOLERANCE}" + "${ABSOLUTE_RESTART_TOLERANCE}") + set_property(TEST TestSimulationSheathRestart_xperiod_vx_user_defined_grid PROPERTY TIMEOUT 200) + set_property(TEST TestSimulationSheathRestart_xperiod_vx_user_defined_grid PROPERTY COST 100) +endif() diff --git a/tests/geometryXVx/sheath/test_sheath_restart.sh b/tests/geometryXVx/sheath/test_sheath_restart.sh new file mode 100644 index 000000000..bcca4dcae --- /dev/null +++ b/tests/geometryXVx/sheath/test_sheath_restart.sh @@ -0,0 +1,71 @@ +#!/bin/bash +set -xe + +if [ $# -lt 4 ] || [ $# -gt 6 ] +then + echo "Usage: $0 [ ]" + exit 1 +fi +VOICEXX_SRCDIR="$1" +VOICEXX_EXEC="$2" +PYTHON3_EXE="$3" +SIMULATION_NAME="$4" +if [ -n "$5" ] +then + RELATIVE_RESTART_TOLERANCE="$5" +fi +if [ -n "$6" ] +then + ABSOLUTE_RESTART_TOLERANCE="$6" +fi + +OUTDIR="${PWD}/${SIMULATION_NAME}" + +TMPDIR="$(mktemp -p "${PWD}" -d run-XXXXXXXXXX)" +function finish { + rm -rf "${TMPDIR}" +} +trap finish EXIT QUIT ABRT KILL SEGV TERM STOP + +cd "$(dirname "$0")" +TESTDIR="${PWD}" + +cd "${TMPDIR}" + +RSTDIR="${TMPDIR}/RST" +mkdir "${RSTDIR}" +cd "${RSTDIR}" + +"${VOICEXX_EXEC}" "--dump-config" "${PWD}/sheath.yaml" +sed -i 's/^ x_ncells: .*/ x_ncells: 16/' sheath.yaml +sed -i 's/^ vx_ncells: .*/ vx_ncells: 16/' sheath.yaml +sed -i 's/^ nbiter: .*/ nbiter: 10/' sheath.yaml +sed -i 's/^ deltat: .*/ deltat: 0.125/' sheath.yaml +sed -i 's/^ time_diag: .*/ time_diag: 0.25/' sheath.yaml + +"${VOICEXX_EXEC}" "${PWD}/sheath.yaml" + +cd "${TMPDIR}" +cp "${RSTDIR}/VOICEXX_initstate.h5" . +cp "${RSTDIR}/VOICEXX_00003.h5" . +cp "${RSTDIR}/sheath.yaml" sheath_restart.yaml + +"${VOICEXX_EXEC}" --iter-restart 3 "${PWD}/sheath_restart.yaml" +sed -i 's/^ nbiter: .*/ nbiter: 2/' sheath_restart.yaml +sed -i 's/^ time_diag: .*/ time_diag: 0.5/' sheath_restart.yaml + +h5ls -d ${PWD}/VOICEXX_00005.h5/time_saved ${RSTDIR}/VOICEXX_00005.h5/time_saved +${PYTHON3_EXE} ${VOICEXX_SRCDIR}/post-process/PythonScripts/compare_hdf5_results.py ${PWD}/VOICEXX_00005.h5 ${RSTDIR}/VOICEXX_00005.h5 time_saved -R ${RELATIVE_RESTART_TOLERANCE} -A ${ABSOLUTE_RESTART_TOLERANCE} +if [ $? -ne 0 ]; then + exit 1 +fi + +${PYTHON3_EXE} ${VOICEXX_SRCDIR}/post-process/PythonScripts/compare_hdf5_results.py ${PWD}/VOICEXX_00005.h5 ${RSTDIR}/VOICEXX_00005.h5 electrostatic_potential -R ${RELATIVE_RESTART_TOLERANCE} -A ${ABSOLUTE_RESTART_TOLERANCE} +if [ $? -ne 0 ]; then + exit 1 +fi + +${PYTHON3_EXE} ${VOICEXX_SRCDIR}/post-process/PythonScripts/compare_hdf5_results.py ${PWD}/VOICEXX_00005.h5 ${RSTDIR}/VOICEXX_00005.h5 fdistribu -R ${RELATIVE_RESTART_TOLERANCE} -A ${ABSOLUTE_RESTART_TOLERANCE} +if [ $? -ne 0 ]; then + exit 1 +fi diff --git a/tests/geometryXVx/sheath/test_sheath_restart_user_defined_grid.sh b/tests/geometryXVx/sheath/test_sheath_restart_user_defined_grid.sh new file mode 100644 index 000000000..40480f14d --- /dev/null +++ b/tests/geometryXVx/sheath/test_sheath_restart_user_defined_grid.sh @@ -0,0 +1,75 @@ +#!/bin/bash +set -xe + +if [ $# -lt 4 ] || [ $# -gt 6 ] +then + echo "Usage: $0 [ ]" + exit 1 +fi +VOICEXX_SRCDIR="$1" +VOICEXX_EXEC="$2" +PYTHON3_EXE="$3" +SIMULATION_NAME="$4" +if [ -n "$5" ] +then + RELATIVE_RESTART_TOLERANCE="$5" +fi +if [ -n "$6" ] +then + ABSOLUTE_RESTART_TOLERANCE="$6" +fi + +OUTDIR="${PWD}/${SIMULATION_NAME}" + +TMPDIR="$(mktemp -p "${PWD}" -d run-XXXXXXXXXX)" +function finish { + rm -rf "${TMPDIR}" +} +trap finish EXIT QUIT ABRT KILL SEGV TERM STOP + +cd "$(dirname "$0")" +TESTDIR="${PWD}" + +cd "${TMPDIR}" + +RSTDIR="${TMPDIR}/RST" +mkdir "${RSTDIR}" +cd "${RSTDIR}" + +${PYTHON3_EXE} ${VOICEXX_SRCDIR}/pre-process/PythonScripts/geometryXVx/suggested_points_refinement.py ${RSTDIR}/grids.h5 --edge-domains 0.0 50.0 --ncells 16 --name grid_x --periodic --xmin 0.0 --xmax 50.0 +${PYTHON3_EXE} ${VOICEXX_SRCDIR}/pre-process/PythonScripts/geometryXVx/suggested_points_refinement.py ${RSTDIR}/grids.h5 --edge-domains -6.0 6.0 --ncells 16 --name grid_vx + +"${VOICEXX_EXEC}" "--dump-config" "${PWD}/sheath.yaml" +sed -i 's/^ x_ncells: .*/ x_ncells: 16/' sheath.yaml +sed -i 's/^ vx_ncells: .*/ vx_ncells: 16/' sheath.yaml +sed -i 's/^ nbiter: .*/ nbiter: 10/' sheath.yaml +sed -i 's/^ deltat: .*/ deltat: 0.125/' sheath.yaml +sed -i 's/^ time_diag: .*/ time_diag: 0.25/' sheath.yaml + +"${VOICEXX_EXEC}" "${PWD}/sheath.yaml" + +cd "${TMPDIR}" +cp "${RSTDIR}/VOICEXX_initstate.h5" . +cp "${RSTDIR}/VOICEXX_00003.h5" . +cp "${RSTDIR}/sheath.yaml" sheath_restart.yaml +cp "${RSTDIR}/grids.h5" . + +"${VOICEXX_EXEC}" --iter-restart 3 "${PWD}/sheath_restart.yaml" +sed -i 's/^ nbiter: .*/ nbiter: 2/' sheath_restart.yaml +sed -i 's/^ time_diag: .*/ time_diag: 0.5/' sheath_restart.yaml + +h5ls -d ${PWD}/VOICEXX_00005.h5/time_saved ${RSTDIR}/VOICEXX_00005.h5/time_saved +${PYTHON3_EXE} ${VOICEXX_SRCDIR}/post-process/PythonScripts/compare_hdf5_results.py ${PWD}/VOICEXX_00005.h5 ${RSTDIR}/VOICEXX_00005.h5 time_saved -R ${RELATIVE_RESTART_TOLERANCE} -A ${ABSOLUTE_RESTART_TOLERANCE} +if [ $? -ne 0 ]; then + exit 1 +fi + +${PYTHON3_EXE} ${VOICEXX_SRCDIR}/post-process/PythonScripts/compare_hdf5_results.py ${PWD}/VOICEXX_00005.h5 ${RSTDIR}/VOICEXX_00005.h5 electrostatic_potential -R ${RELATIVE_RESTART_TOLERANCE} -A ${ABSOLUTE_RESTART_TOLERANCE} +if [ $? -ne 0 ]; then + exit 1 +fi + +${PYTHON3_EXE} ${VOICEXX_SRCDIR}/post-process/PythonScripts/compare_hdf5_results.py ${PWD}/VOICEXX_00005.h5 ${RSTDIR}/VOICEXX_00005.h5 fdistribu -R ${RELATIVE_RESTART_TOLERANCE} -A ${ABSOLUTE_RESTART_TOLERANCE} +if [ $? -ne 0 ]; then + exit 1 +fi