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* baseline implementation of the curvilinear USBP for testing * working version of curvilinear upwind solver. Needs significant cleanup of debugging statements and different variants of the rotated flux vector splittings * cleanup of the fdsbp_2d file * clean-up FVS routines in the compressible Euler file * cleanup and remove unnecessary containers * add tests for the new solver * remove extra space * run formatter * Apply suggestions from code review Co-authored-by: Hendrik Ranocha <[email protected]> * add specialized calc_metric_terms function for upwind type * revert change to the surface integral function * add reference for curvilinear van Leer splitting * new splitting_drikakis_tsangaris in Cartesian and generalized coordinates * added test for Cartesian splitting_drikakis_tsangaris * run formatter * Update src/equations/compressible_euler_2d.jl * remove orientation_or_normal from Steger-Warming --------- Co-authored-by: Hendrik Ranocha <[email protected]>
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examples/unstructured_2d_fdsbp/elixir_euler_free_stream_upwind.jl
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# !!! warning "Experimental implementation (upwind SBP)" | ||
# This is an experimental feature and may change in future releases. | ||
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the compressible Euler equations | ||
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equations = CompressibleEulerEquations2D(1.4) | ||
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initial_condition = initial_condition_constant | ||
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# Boundary conditions for free-stream preservation test | ||
boundary_condition_free_stream = BoundaryConditionDirichlet(initial_condition) | ||
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boundary_conditions = Dict(:outerCircle => boundary_condition_free_stream, | ||
:cone1 => boundary_condition_free_stream, | ||
:cone2 => boundary_condition_free_stream, | ||
:iceCream => boundary_condition_free_stream) | ||
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############################################################################### | ||
# Get the Upwind FDSBP approximation space | ||
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# TODO: FDSBP | ||
# Note, one must set `xmin=-1` and `xmax=1` due to the reuse | ||
# of interpolation routines from `calc_node_coordinates!` to create | ||
# the physical coordinates in the mappings. | ||
D_upw = upwind_operators(SummationByPartsOperators.Mattsson2017, | ||
derivative_order = 1, | ||
accuracy_order = 8, | ||
xmin = -1.0, xmax = 1.0, | ||
N = 17) | ||
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flux_splitting = splitting_vanleer_haenel | ||
solver = FDSBP(D_upw, | ||
surface_integral = SurfaceIntegralStrongForm(FluxUpwind(flux_splitting)), | ||
volume_integral = VolumeIntegralUpwind(flux_splitting)) | ||
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############################################################################### | ||
# Get the curved quad mesh from a file (downloads the file if not available locally) | ||
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# Mesh with second-order boundary polynomials requires an upwind SBP operator | ||
# with (at least) 4th order boundary closure to guarantee the approximation is | ||
# free-stream preserving | ||
mesh_file = Trixi.download("https://gist.githubusercontent.com/andrewwinters5000/ec9a345f09199ebe471d35d5c1e4e08f/raw/15975943d8642e42f8292235314b6f1b30aa860d/mesh_inner_outer_boundaries.mesh", | ||
joinpath(@__DIR__, "mesh_inner_outer_boundaries.mesh")) | ||
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mesh = UnstructuredMesh2D(mesh_file) | ||
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############################################################################### | ||
# create the semi discretization object | ||
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semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver, | ||
boundary_conditions = boundary_conditions) | ||
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############################################################################### | ||
# ODE solvers, callbacks etc. | ||
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tspan = (0.0, 5.0) | ||
ode = semidiscretize(semi, tspan) | ||
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summary_callback = SummaryCallback() | ||
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analysis_interval = 1000 | ||
analysis_callback = AnalysisCallback(semi, interval = analysis_interval) | ||
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alive_callback = AliveCallback(analysis_interval = analysis_interval) | ||
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save_solution = SaveSolutionCallback(interval = 1000, | ||
save_initial_solution = true, | ||
save_final_solution = true) | ||
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callbacks = CallbackSet(summary_callback, | ||
analysis_callback, | ||
save_solution, | ||
alive_callback) | ||
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############################################################################### | ||
# run the simulation | ||
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# set small tolerances for the free-stream preservation test | ||
sol = solve(ode, SSPRK43(), abstol = 1.0e-12, reltol = 1.0e-12, | ||
save_everystep = false, callback = callbacks) | ||
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summary_callback() # print the timer summary |
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examples/unstructured_2d_fdsbp/elixir_euler_source_terms_upwind.jl
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@@ -0,0 +1,87 @@ | ||
# !!! warning "Experimental implementation (upwind SBP)" | ||
# This is an experimental feature and may change in future releases. | ||
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the compressible Euler equations | ||
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equations = CompressibleEulerEquations2D(1.4) | ||
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initial_condition = initial_condition_convergence_test | ||
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source_term = source_terms_convergence_test | ||
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boundary_condition_eoc = BoundaryConditionDirichlet(initial_condition) | ||
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boundary_conditions = Dict(:Top => boundary_condition_eoc, | ||
:Bottom => boundary_condition_eoc, | ||
:Right => boundary_condition_eoc, | ||
:Left => boundary_condition_eoc) | ||
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############################################################################### | ||
# Get the Upwind FDSBP approximation space | ||
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# TODO: FDSBP | ||
# Note, one must set `xmin=-1` and `xmax=1` due to the reuse | ||
# of interpolation routines from `calc_node_coordinates!` to create | ||
# the physical coordinates in the mappings. | ||
D_upw = upwind_operators(SummationByPartsOperators.Mattsson2017, | ||
derivative_order = 1, | ||
accuracy_order = 4, | ||
xmin = -1.0, xmax = 1.0, | ||
N = 9) | ||
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flux_splitting = splitting_drikakis_tsangaris | ||
solver = FDSBP(D_upw, | ||
surface_integral = SurfaceIntegralStrongForm(FluxUpwind(flux_splitting)), | ||
volume_integral = VolumeIntegralUpwind(flux_splitting)) | ||
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############################################################################### | ||
# Get the curved quad mesh from a file (downloads the file if not available locally) | ||
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# Mesh with first-order boundary polynomials requires an upwind SBP operator | ||
# with (at least) 2nd order boundary closure to guarantee the approximation is | ||
# free-stream preserving | ||
mesh_file = Trixi.download("https://gist.githubusercontent.com/andrewwinters5000/a4f4743008bf3233957a9ea6ac7a62e0/raw/8b36cc6649153fe0a5723b200368a210a1d74eaf/mesh_refined_box.mesh", | ||
joinpath(@__DIR__, "mesh_refined_box.mesh")) | ||
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mesh = UnstructuredMesh2D(mesh_file) | ||
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############################################################################### | ||
# create the semidiscretization object | ||
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semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver, | ||
source_terms = source_term, | ||
boundary_conditions = boundary_conditions) | ||
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############################################################################### | ||
# ODE solvers, callbacks etc. | ||
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tspan = (0.0, 1.0) | ||
ode = semidiscretize(semi, tspan) | ||
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summary_callback = SummaryCallback() | ||
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analysis_interval = 1000 | ||
analysis_callback = AnalysisCallback(semi, interval = analysis_interval) | ||
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alive_callback = AliveCallback(analysis_interval = analysis_interval) | ||
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save_solution = SaveSolutionCallback(interval = 1000, | ||
save_initial_solution = true, | ||
save_final_solution = true) | ||
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callbacks = CallbackSet(summary_callback, | ||
analysis_callback, | ||
save_solution, | ||
alive_callback) | ||
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############################################################################### | ||
# run the simulation | ||
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sol = solve(ode, SSPRK43(), abstol = 1.0e-6, reltol = 1.0e-6, | ||
save_everystep = false, callback = callbacks) | ||
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summary_callback() # print the timer summary |
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