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name = "Trixi" | ||
uuid = "a7f1ee26-1774-49b1-8366-f1abc58fbfcb" | ||
authors = ["Michael Schlottke-Lakemper <[email protected]>", "Gregor Gassner <[email protected]>", "Hendrik Ranocha <[email protected]>", "Andrew R. Winters <[email protected]>", "Jesse Chan <[email protected]>"] | ||
version = "0.7.1-pre" | ||
version = "0.7.2-pre" | ||
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[deps] | ||
CodeTracking = "da1fd8a2-8d9e-5ec2-8556-3022fb5608a2" | ||
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86
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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# !!! 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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