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trixi-framework / Trixi.jl / 22503087308

27 Feb 2026 08:43PM UTC coverage: 85.574% (-11.6%) from 97.128%
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Avoid repeated global memory operations in `prolong2interfaces!` for Gauss nodes (#2830)

* prolong2interfaces! 1D

* 2D

* Apply suggestions from code review

---------

Co-authored-by: Daniel Doehring <daniel.doehring@rwth-aachen.de>

12 of 18 new or added lines in 2 files covered. (66.67%)

5301 existing lines in 247 files now uncovered.

39316 of 45944 relevant lines covered (85.57%)

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0.0
/examples/structured_3d_dgsem/elixir_euler_source_terms.jl
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# The same setup as tree_3d_dgsem/elixir_euler_source_terms.jl
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# to verify the StructuredMesh implementation against TreeMesh
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using OrdinaryDiffEqLowStorageRK
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using Trixi
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###############################################################################
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# semidiscretization of the compressible Euler equations
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equations = CompressibleEulerEquations3D(1.4)
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initial_condition = initial_condition_convergence_test
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# Up to version 0.13.0, `max_abs_speed_naive` was used as the default wave speed estimate of
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# `const flux_lax_friedrichs = FluxLaxFriedrichs(), i.e., `FluxLaxFriedrichs(max_abs_speed = max_abs_speed_naive)`.
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# In the `StepsizeCallback`, though, the less diffusive `max_abs_speeds` is employed which is consistent with `max_abs_speed`.
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# Thus, we exchanged in PR#2458 the default wave speed used in the LLF flux to `max_abs_speed`.
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# To ensure that every example still runs we specify explicitly `FluxLaxFriedrichs(max_abs_speed_naive)`.
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# We remark, however, that the now default `max_abs_speed` is in general recommended due to compliance with the
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# `StepsizeCallback` (CFL-Condition) and less diffusion.
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solver = DGSEM(polydeg = 3, surface_flux = FluxLaxFriedrichs(max_abs_speed_naive),
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               volume_integral = VolumeIntegralWeakForm())
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# coordinates_min = (0.0, 0.0, 0.0)
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# coordinates_max = (2.0, 2.0, 2.0)
UNCOV
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f1(s, t) = SVector(0.0, s + 1.0, t + 1.0)
×
UNCOV
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f2(s, t) = SVector(2.0, s + 1.0, t + 1.0)
×
UNCOV
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f3(s, t) = SVector(s + 1.0, 0.0, t + 1.0)
×
UNCOV
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f4(s, t) = SVector(s + 1.0, 2.0, t + 1.0)
×
UNCOV
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f5(s, t) = SVector(s + 1.0, t + 1.0, 0.0)
×
UNCOV
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f6(s, t) = SVector(s + 1.0, t + 1.0, 2.0)
×
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cells_per_dimension = (4, 4, 4)
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mesh = StructuredMesh(cells_per_dimension, (f1, f2, f3, f4, f5, f6), periodicity = true)
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semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver;
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                                    source_terms = source_terms_convergence_test,
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                                    boundary_conditions = boundary_condition_periodic)
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###############################################################################
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# ODE solvers, callbacks etc.
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tspan = (0.0, 5.0)
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ode = semidiscretize(semi, tspan)
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summary_callback = SummaryCallback()
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analysis_interval = 100
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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 = 100,
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                                     save_initial_solution = true,
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                                     save_final_solution = true,
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                                     solution_variables = cons2prim)
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stepsize_callback = StepsizeCallback(cfl = 0.6)
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callbacks = CallbackSet(summary_callback,
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                        analysis_callback, alive_callback,
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                        save_solution,
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                        stepsize_callback)
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###############################################################################
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# run the simulation
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sol = solve(ode, CarpenterKennedy2N54(williamson_condition = false);
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            dt = 1.0, # solve needs some value here but it will be overwritten by the stepsize_callback
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            ode_default_options()..., callback = callbacks);
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