Path: blob/main/examples/dgmulti_2d/elixir_navierstokes_lid_driven_cavity.jl
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using OrdinaryDiffEqLowStorageRK1using Trixi23###############################################################################4# semidiscretization of the ideal compressible Navier-Stokes equations56prandtl_number() = 0.727mu = 0.00189equations = CompressibleEulerEquations2D(1.4)10equations_parabolic = CompressibleNavierStokesDiffusion2D(equations, mu = mu,11Prandtl = prandtl_number())1213# Create DG solver with polynomial degree = 3 and (local) Lax-Friedrichs/Rusanov flux as surface flux1415# Up to version 0.13.0, `max_abs_speed_naive` was used as the default wave speed estimate of16# `const flux_lax_friedrichs = FluxLaxFriedrichs(), i.e., `FluxLaxFriedrichs(max_abs_speed = max_abs_speed_naive)`.17# In the `StepsizeCallback`, though, the less diffusive `max_abs_speeds` is employed which is consistent with `max_abs_speed`.18# Thus, we exchanged in PR#2458 the default wave speed used in the LLF flux to `max_abs_speed`.19# To ensure that every example still runs we specify explicitly `FluxLaxFriedrichs(max_abs_speed_naive)`.20# We remark, however, that the now default `max_abs_speed` is in general recommended due to compliance with the21# `StepsizeCallback` (CFL-Condition) and less diffusion.22dg = DGMulti(polydeg = 3, element_type = Quad(), approximation_type = GaussSBP(),23surface_integral = SurfaceIntegralWeakForm(FluxLaxFriedrichs(max_abs_speed_naive)),24volume_integral = VolumeIntegralFluxDifferencing(flux_ranocha))2526top(x, tol = 50 * eps()) = abs(x[2] - 1) < tol27rest_of_boundary(x, tol = 50 * eps()) = !top(x, tol)28is_on_boundary = Dict(:top => top, :rest_of_boundary => rest_of_boundary)2930cells_per_dimension = (16, 16)31mesh = DGMultiMesh(dg, cells_per_dimension; is_on_boundary)3233function initial_condition_cavity(x, t, equations::CompressibleEulerEquations2D)34Ma = 0.135rho = 1.036u, v = 0.0, 0.037p = 1.0 / (Ma^2 * equations.gamma)38return prim2cons(SVector(rho, u, v, p), equations)39end40initial_condition = initial_condition_cavity4142# BC types43velocity_bc_lid = NoSlip((x, t, equations_parabolic) -> SVector(1.0, 0.0))44velocity_bc_cavity = NoSlip((x, t, equations_parabolic) -> SVector(0.0, 0.0))45heat_bc = Adiabatic((x, t, equations_parabolic) -> 0.0)46boundary_condition_lid = BoundaryConditionNavierStokesWall(velocity_bc_lid, heat_bc)47boundary_condition_cavity = BoundaryConditionNavierStokesWall(velocity_bc_cavity, heat_bc)4849# define inviscid boundary conditions50boundary_conditions = (; :top => boundary_condition_slip_wall,51:rest_of_boundary => boundary_condition_slip_wall)5253# define viscous boundary conditions54boundary_conditions_parabolic = (; :top => boundary_condition_lid,55:rest_of_boundary => boundary_condition_cavity)5657semi = SemidiscretizationHyperbolicParabolic(mesh, (equations, equations_parabolic),58initial_condition, dg;59boundary_conditions = (boundary_conditions,60boundary_conditions_parabolic))6162###############################################################################63# ODE solvers, callbacks etc.6465# Create ODE problem with time span `tspan`66tspan = (0.0, 10.0)67ode = semidiscretize(semi, tspan)6869summary_callback = SummaryCallback()70alive_callback = AliveCallback(alive_interval = 10)71analysis_interval = 10072analysis_callback = AnalysisCallback(semi, interval = analysis_interval, uEltype = real(dg))73save_solution = SaveSolutionCallback(interval = analysis_interval,74solution_variables = cons2prim)75callbacks = CallbackSet(summary_callback, alive_callback, analysis_callback, save_solution)7677###############################################################################78# run the simulation7980time_int_tol = 1e-881sol = solve(ode, RDPK3SpFSAL49(); abstol = time_int_tol, reltol = time_int_tol,82ode_default_options()..., callback = callbacks)838485