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Implement 3D support for
P4estMesh
(#637)
* Implement structured 3D simulations with P4estMesh * Fix loading and saving of P4estMesh in 3D * Fix unstructured P4estMesh simulation in 3D * Revise 3D orientations * Implement P4estMesh simulation for non-conforming 3D meshes * Add non-conforming example * Clean up * Remove unused destroy functions * Clean up more * Add restart example with P4estMesh in 3D * Implement AMR with P4estMesh in 3D * Add AMR example with P4estMesh in 3D * First version of fast calc_contravariant_vectors! * Make calc_contravariant_vectors! more readable * Improve documentation of calc_contravariant_vectors! * Calculate both summands of contravariant vectors in one loop * Move @turbo to inner loop * Only use one loop over n * Optimize calc_jacobian_matrix! * Optimize calc_inverse_jacobian! * Use tmp arrays for multiply_dimensionwise! * Update Euler FSP errors after optimizing code * Remove duplicate code * Dispatch by function type * Compute contravariant vectors in one loop for each summand * Add more 3D `P4estMesh` examples * Make curved example actually curved * Make calc_node_coordinates! consistent with 2D * Remove sign Jacobian from normal vector p4est doesn't support left-handed coordinates anyway. * Add FSP example with P4estMesh * Add P4estMesh examples to tests * Clean up * Update examples/3d/elixir_advection_amr_p4est.jl Co-authored-by: Hendrik Ranocha <[email protected]> * Update examples/3d/elixir_advection_basic_p4est.jl Co-authored-by: Hendrik Ranocha <[email protected]> * Update src/solvers/dg_p4est/containers_2d.jl Co-authored-by: Hendrik Ranocha <[email protected]> * Only use Base functions for sc_array load and wrap * Implement suggestions * Implement suggestions * Add convergence test for 3D `P4estMesh` * Implement suggestions Co-authored-by: Hendrik Ranocha <[email protected]>
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the linear advection equation | ||
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advectionvelocity = (0.2, -0.7, 0.5) | ||
equations = LinearScalarAdvectionEquation3D(advectionvelocity) | ||
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initial_condition = initial_condition_gauss | ||
solver = DGSEM(polydeg=3, surface_flux=flux_lax_friedrichs) | ||
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coordinates_min = (-5, -5, -5) | ||
coordinates_max = ( 5, 5, 5) | ||
trees_per_dimension = (1, 1, 1) | ||
mesh = P4estMesh(trees_per_dimension, polydeg=1, | ||
coordinates_min=coordinates_min, coordinates_max=coordinates_max, | ||
initial_refinement_level=4) | ||
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semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver) | ||
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############################################################################### | ||
# ODE solvers, callbacks etc. | ||
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tspan = (0.0, 0.3) | ||
ode = semidiscretize(semi, tspan) | ||
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summary_callback = SummaryCallback() | ||
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analysis_interval = 100 | ||
analysis_callback = AnalysisCallback(semi, interval=analysis_interval, | ||
extra_analysis_integrals=(entropy,)) | ||
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alive_callback = AliveCallback(analysis_interval=analysis_interval) | ||
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save_restart = SaveRestartCallback(interval=100, | ||
save_final_restart=true) | ||
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save_solution = SaveSolutionCallback(interval=100, | ||
save_initial_solution=true, | ||
save_final_solution=true, | ||
solution_variables=cons2prim) | ||
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amr_controller = ControllerThreeLevel(semi, IndicatorMax(semi, variable=first), | ||
base_level=4, | ||
med_level=5, med_threshold=0.1, | ||
max_level=6, max_threshold=0.6) | ||
amr_callback = AMRCallback(semi, amr_controller, | ||
interval=5, | ||
adapt_initial_condition=true, | ||
adapt_initial_condition_only_refine=true) | ||
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stepsize_callback = StepsizeCallback(cfl=1.2) | ||
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callbacks = CallbackSet(summary_callback, | ||
analysis_callback, | ||
alive_callback, | ||
save_restart, | ||
save_solution, | ||
amr_callback, | ||
stepsize_callback) | ||
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############################################################################### | ||
# run the simulation | ||
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sol = solve(ode, CarpenterKennedy2N54(williamson_condition=false), | ||
dt=1.0, # solve needs some value here but it will be overwritten by the stepsize_callback | ||
save_everystep=false, callback=callbacks); | ||
summary_callback() # print the timer summary |
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105
examples/3d/elixir_advection_amr_p4est_unstructured_curved.jl
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the linear advection equation | ||
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advectionvelocity = (0.2, -0.7, 0.5) | ||
equations = LinearScalarAdvectionEquation3D(advectionvelocity) | ||
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solver = DGSEM(polydeg=3, surface_flux=flux_lax_friedrichs) | ||
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initial_condition = initial_condition_gauss | ||
boundary_condition = BoundaryConditionDirichlet(initial_condition) | ||
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boundary_conditions = Dict( | ||
:all => boundary_condition | ||
) | ||
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# Mapping as described in https://arxiv.org/abs/2012.12040, but with less warping. | ||
# The original mapping applied to this unstructured mesh creates extreme angles, | ||
# which require a high resolution for proper results. | ||
function mapping(xi, eta, zeta) | ||
# Don't transform input variables between -1 and 1 onto [0,3] to obtain curved boundaries | ||
# xi = 1.5 * xi_ + 1.5 | ||
# eta = 1.5 * eta_ + 1.5 | ||
# zeta = 1.5 * zeta_ + 1.5 | ||
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y = eta + 1/4 * (cos(1.5 * pi * (2 * xi - 3)/3) * | ||
cos(0.5 * pi * (2 * eta - 3)/3) * | ||
cos(0.5 * pi * (2 * zeta - 3)/3)) | ||
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x = xi + 1/4 * (cos(0.5 * pi * (2 * xi - 3)/3) * | ||
cos(2 * pi * (2 * y - 3)/3) * | ||
cos(0.5 * pi * (2 * zeta - 3)/3)) | ||
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z = zeta + 1/4 * (cos(0.5 * pi * (2 * x - 3)/3) * | ||
cos(pi * (2 * y - 3)/3) * | ||
cos(0.5 * pi * (2 * zeta - 3)/3)) | ||
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# Transform the weird deformed cube to be approximately the size of [-5,5]^3 to match IC | ||
return SVector(5 * x, 5 * y, 5 * z) | ||
end | ||
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# Unstructured mesh with 48 cells of the cube domain [-1, 1]^3 | ||
mesh_file = joinpath(@__DIR__, "cube_unstructured_2.inp") | ||
isfile(mesh_file) || download("https://gist.githubusercontent.com/efaulhaber/b8df0033798e4926dec515fc045e8c2c/raw/b9254cde1d1fb64b6acc8416bc5ccdd77a240227/cube_unstructured_2.inp", | ||
mesh_file) | ||
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mesh = P4estMesh{3}(mesh_file, polydeg=3, | ||
mapping=mapping, | ||
initial_refinement_level=1) | ||
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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, 8.0) | ||
ode = semidiscretize(semi, tspan) | ||
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summary_callback = SummaryCallback() | ||
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analysis_interval = 100 | ||
analysis_callback = AnalysisCallback(semi, interval=analysis_interval, | ||
extra_analysis_integrals=(entropy,)) | ||
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alive_callback = AliveCallback(analysis_interval=analysis_interval) | ||
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save_restart = SaveRestartCallback(interval=100, | ||
save_final_restart=true) | ||
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save_solution = SaveSolutionCallback(interval=100, | ||
save_initial_solution=true, | ||
save_final_solution=true, | ||
solution_variables=cons2prim) | ||
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amr_controller = ControllerThreeLevel(semi, IndicatorMax(semi, variable=first), | ||
base_level=1, | ||
med_level=2, med_threshold=0.1, | ||
max_level=3, max_threshold=0.6) | ||
amr_callback = AMRCallback(semi, amr_controller, | ||
interval=5, | ||
adapt_initial_condition=true, | ||
adapt_initial_condition_only_refine=true) | ||
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stepsize_callback = StepsizeCallback(cfl=1.2) | ||
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callbacks = CallbackSet(summary_callback, | ||
analysis_callback, | ||
alive_callback, | ||
save_restart, | ||
save_solution, | ||
amr_callback, | ||
stepsize_callback) | ||
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############################################################################### | ||
# run the simulation | ||
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sol = solve(ode, CarpenterKennedy2N54(williamson_condition=false), | ||
dt=1.0, # solve needs some value here but it will be overwritten by the stepsize_callback | ||
save_everystep=false, callback=callbacks); | ||
summary_callback() # print the timer summary |
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Original file line number | Diff line number | Diff line change |
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the linear advection equation | ||
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advectionvelocity = (1.0, 1.0, 1.0) | ||
equations = LinearScalarAdvectionEquation3D(advectionvelocity) | ||
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# Create DG solver with polynomial degree = 3 and (local) Lax-Friedrichs/Rusanov flux as surface flux | ||
solver = DGSEM(polydeg=3, surface_flux=flux_lax_friedrichs) | ||
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coordinates_min = (-1.5, -0.9, 0.0) # minimum coordinates (min(x), min(y), min(z)) | ||
coordinates_max = ( 0.5, 1.1, 4.0) # maximum coordinates (max(x), max(y), max(z)) | ||
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# Create P4estMesh with 8 x 10 x 16 elements (note `refinement_level=1`) | ||
trees_per_dimension = (4, 5, 8) | ||
mesh = P4estMesh(trees_per_dimension, polydeg=3, | ||
coordinates_min=coordinates_min, coordinates_max=coordinates_max, | ||
initial_refinement_level=1) | ||
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# A semidiscretization collects data structures and functions for the spatial discretization | ||
semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition_convergence_test, solver) | ||
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############################################################################### | ||
# ODE solvers, callbacks etc. | ||
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# Create ODE problem with time span from 0.0 to 1.0 | ||
ode = semidiscretize(semi, (0.0, 1.0)); | ||
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# At the beginning of the main loop, the SummaryCallback prints a summary of the simulation setup | ||
# and resets the timers | ||
summary_callback = SummaryCallback() | ||
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# The AnalysisCallback allows to analyse the solution in regular intervals and prints the results | ||
analysis_callback = AnalysisCallback(semi, interval=100) | ||
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# The SaveRestartCallback allows to save a file from which a Trixi simulation can be restarted | ||
save_restart = SaveRestartCallback(interval=100, | ||
save_final_restart=true) | ||
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# The SaveSolutionCallback allows to save the solution to a file in regular intervals | ||
save_solution = SaveSolutionCallback(interval=100, | ||
solution_variables=cons2prim) | ||
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# The StepsizeCallback handles the re-calculcation of the maximum Δt after each time step | ||
stepsize_callback = StepsizeCallback(cfl=1.2) | ||
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# Create a CallbackSet to collect all callbacks such that they can be passed to the ODE solver | ||
callbacks = CallbackSet(summary_callback, analysis_callback, save_restart, save_solution, stepsize_callback) | ||
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############################################################################### | ||
# run the simulation | ||
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# OrdinaryDiffEq's `solve` method evolves the solution in time and executes the passed callbacks | ||
sol = solve(ode, CarpenterKennedy2N54(williamson_condition=false), | ||
dt=1.0, # solve needs some value here but it will be overwritten by the stepsize_callback | ||
save_everystep=false, callback=callbacks); | ||
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# Print the timer summary | ||
summary_callback() |
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Original file line number | Diff line number | Diff line change |
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@@ -0,0 +1,76 @@ | ||
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the linear advection equation | ||
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advectionvelocity = (1.0, 1.0, 1.0) | ||
equations = LinearScalarAdvectionEquation3D(advectionvelocity) | ||
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# Create DG solver with polynomial degree = 3 and (local) Lax-Friedrichs/Rusanov flux as surface flux | ||
solver = DGSEM(polydeg=3, surface_flux=flux_lax_friedrichs) | ||
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coordinates_min = (-1.0, -1.0, -1.0) # minimum coordinates (min(x), min(y), min(z)) | ||
coordinates_max = ( 1.0, 1.0, 1.0) # maximum coordinates (max(x), max(y), max(z)) | ||
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trees_per_dimension = (1, 1, 1) | ||
mesh = P4estMesh(trees_per_dimension, polydeg=3, | ||
coordinates_min=coordinates_min, coordinates_max=coordinates_max, | ||
initial_refinement_level=2) | ||
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# Refine bottom left quadrant of each tree to level 4 | ||
function refine_fn(p8est, which_tree, quadrant) | ||
if quadrant.x == 0 && quadrant.y == 0 && quadrant.z == 0 && quadrant.level < 3 | ||
# return true (refine) | ||
return Cint(1) | ||
else | ||
# return false (don't refine) | ||
return Cint(0) | ||
end | ||
end | ||
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# Refine recursively until each bottom left quadrant of a tree has level 2 | ||
# The mesh will be rebalanced before the simulation starts | ||
refine_fn_c = @cfunction(refine_fn, Cint, (Ptr{Trixi.p8est_t}, Ptr{Trixi.p4est_topidx_t}, Ptr{Trixi.p8est_quadrant_t})) | ||
Trixi.refine_p4est!(mesh.p4est, true, refine_fn_c, C_NULL) | ||
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# A semidiscretization collects data structures and functions for the spatial discretization | ||
semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition_convergence_test, solver) | ||
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############################################################################### | ||
# ODE solvers, callbacks etc. | ||
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# Create ODE problem with time span from 0.0 to 1.0 | ||
ode = semidiscretize(semi, (0.0, 1.0)); | ||
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# At the beginning of the main loop, the SummaryCallback prints a summary of the simulation setup | ||
# and resets the timers | ||
summary_callback = SummaryCallback() | ||
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# The AnalysisCallback allows to analyse the solution in regular intervals and prints the results | ||
analysis_callback = AnalysisCallback(semi, interval=100) | ||
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# The SaveSolutionCallback allows to save the solution to a file in regular intervals | ||
save_solution = SaveSolutionCallback(interval=100, | ||
solution_variables=cons2prim) | ||
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# The StepsizeCallback handles the re-calculcation of the maximum Δt after each time step | ||
stepsize_callback = StepsizeCallback(cfl=1.6) | ||
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# Create a CallbackSet to collect all callbacks such that they can be passed to the ODE solver | ||
callbacks = CallbackSet(summary_callback, analysis_callback, save_solution, stepsize_callback) | ||
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############################################################################### | ||
# run the simulation | ||
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# OrdinaryDiffEq's `solve` method evolves the solution in time and executes the passed callbacks | ||
sol = solve(ode, CarpenterKennedy2N54(williamson_condition=false), | ||
dt=1.0, # solve needs some value here but it will be overwritten by the stepsize_callback | ||
save_everystep=false, callback=callbacks); | ||
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# Print the timer summary | ||
summary_callback() |
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