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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 = "0.7.5-pre" | ||
version = "0.7.6-pre" | ||
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[deps] | ||
CodeTracking = "da1fd8a2-8d9e-5ec2-8556-3022fb5608a2" | ||
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@@ -75,7 +75,7 @@ MuladdMacro = "0.2.2" | |
Octavian = "0.3.21" | ||
OffsetArrays = "1.12" | ||
P4est = "0.4.9" | ||
Polyester = "0.7.5" | ||
Polyester = "0.7.10" | ||
PrecompileTools = "1.1" | ||
Preferences = "1.3" | ||
Printf = "1" | ||
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94 changes: 94 additions & 0 deletions
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examples/tree_2d_dgsem/elixir_navierstokes_taylor_green_vortex_sutherland.jl
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the compressible Navier-Stokes equations | ||
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prandtl_number() = 0.72 | ||
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# Use Sutherland's law for a temperature-dependent viscosity. | ||
# For details, see e.g. | ||
# Frank M. White: Viscous Fluid Flow, 2nd Edition. | ||
# 1991, McGraw-Hill, ISBN, 0-07-069712-4 | ||
# Pages 28 and 29. | ||
@inline function mu(u, equations) | ||
T_ref = 291.15 | ||
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R_specific_air = 287.052874 | ||
T = R_specific_air * Trixi.temperature(u, equations) | ||
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C_air = 120.0 | ||
mu_ref_air = 1.827e-5 | ||
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return mu_ref_air * (T_ref + C_air) / (T + C_air) * (T / T_ref)^1.5 | ||
end | ||
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equations = CompressibleEulerEquations2D(1.4) | ||
equations_parabolic = CompressibleNavierStokesDiffusion2D(equations, mu = mu, | ||
Prandtl = prandtl_number()) | ||
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""" | ||
initial_condition_taylor_green_vortex(x, t, equations::CompressibleEulerEquations2D) | ||
The classical viscous Taylor-Green vortex in 2D. | ||
This forms the basis behind the 3D case found for instance in | ||
- Jonathan R. Bull and Antony Jameson | ||
Simulation of the Compressible Taylor Green Vortex using High-Order Flux Reconstruction Schemes | ||
[DOI: 10.2514/6.2014-3210](https://doi.org/10.2514/6.2014-3210) | ||
""" | ||
function initial_condition_taylor_green_vortex(x, t, | ||
equations::CompressibleEulerEquations2D) | ||
A = 1.0 # magnitude of speed | ||
Ms = 0.1 # maximum Mach number | ||
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rho = 1.0 | ||
v1 = A * sin(x[1]) * cos(x[2]) | ||
v2 = -A * cos(x[1]) * sin(x[2]) | ||
p = (A / Ms)^2 * rho / equations.gamma # scaling to get Ms | ||
p = p + 1.0 / 4.0 * A^2 * rho * (cos(2 * x[1]) + cos(2 * x[2])) | ||
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return prim2cons(SVector(rho, v1, v2, p), equations) | ||
end | ||
initial_condition = initial_condition_taylor_green_vortex | ||
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volume_flux = flux_ranocha | ||
solver = DGSEM(polydeg = 3, surface_flux = flux_hllc, | ||
volume_integral = VolumeIntegralFluxDifferencing(volume_flux)) | ||
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coordinates_min = (-1.0, -1.0) .* pi | ||
coordinates_max = (1.0, 1.0) .* pi | ||
mesh = TreeMesh(coordinates_min, coordinates_max, | ||
initial_refinement_level = 4, | ||
n_cells_max = 100_000) | ||
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semi = SemidiscretizationHyperbolicParabolic(mesh, (equations, equations_parabolic), | ||
initial_condition, solver) | ||
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############################################################################### | ||
# ODE solvers, callbacks etc. | ||
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tspan = (0.0, 20.0) | ||
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, | ||
save_analysis = true, | ||
extra_analysis_integrals = (energy_kinetic, | ||
energy_internal)) | ||
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alive_callback = AliveCallback(analysis_interval = analysis_interval) | ||
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callbacks = CallbackSet(summary_callback, | ||
analysis_callback, | ||
alive_callback) | ||
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############################################################################### | ||
# run the simulation | ||
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time_int_tol = 1e-9 | ||
sol = solve(ode, RDPK3SpFSAL49(); abstol = time_int_tol, reltol = time_int_tol, | ||
ode_default_options()..., callback = callbacks) | ||
summary_callback() # print the timer summary |
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