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Compressible Euler Quasi-1D #1757

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deb1fb6
implementation of quasi 1d compressible Euler Equation
KrisshChawla Nov 24, 2023
62734c0
added example elixir for quasi 1d compressible Euler equations
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added example elixir with a discontinuous initial condition
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including and exported CompressibleEulerEquationsQuasi1D
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Merge branch 'main' into compressible_euler_quasi_1d
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Merge branch 'main' into compressible_euler_quasi_1d
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Merge branch 'main' into compressible_euler_quasi_1d
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85 changes: 85 additions & 0 deletions examples/tree_1d_dgsem/elixir_euler_quasi_1d_discontinuous.jl
Original file line number Diff line number Diff line change
@@ -0,0 +1,85 @@
using OrdinaryDiffEq
using Trixi

###############################################################################
# Semidiscretization of the quasi 1d compressible Euler equations
# See Chan et al. https://doi.org/10.48550/arXiv.2307.12089 for details

equations = CompressibleEulerEquationsQuasi1D(1.4)

"""
initial_condition_discontinuity(x, t, equations::CompressibleEulerEquations1D)

An entropy conservation verification initial condition taken from
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- Jesse Chan, Khemraj Shukla, Xinhui Wu, Ruofeng Liu, Prani Nalluri (2023)
High order entropy stable schemes for the quasi-one-dimensional
shallow water and compressible Euler equations
[DOI: 10.48550/arXiv.2307.12089](https://doi.org/10.48550/arXiv.2307.12089)
"""
function initial_condition_discontinuity(x, t,
equations::CompressibleEulerEquationsQuasi1D)
rho = (x[1] < 0) ? 3.4718 : 2.0
v1 = (x[1] < 0) ? -2.5923 : -3.0
p = (x[1] < 0) ? 5.7118 : 2.639
a = (x[1] < 0) ? 1.0 : 1.5

return prim2cons(SVector(rho, v1, p, a), equations)
end

initial_condition = initial_condition_discontinuity

volume_flux = (flux_chan_etal, flux_nonconservative_chan_etal)
surface_flux = (flux_lax_friedrichs, flux_nonconservative_chan_etal)
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basis = LobattoLegendreBasis(3)
indicator_sc = IndicatorHennemannGassner(equations, basis,
alpha_max = 0.5,
alpha_min = 0.001,
alpha_smooth = true,
variable = density_pressure)
volume_integral = VolumeIntegralShockCapturingHG(indicator_sc;
volume_flux_dg = volume_flux,
volume_flux_fv = surface_flux)
solver = DGSEM(basis, surface_flux, volume_integral)

coordinates_min = (-1.0,)
coordinates_max = (1.0,)
mesh = TreeMesh(coordinates_min, coordinates_max,
initial_refinement_level = 6,
n_cells_max = 10_000)

semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver)

###############################################################################
# ODE solvers, callbacks etc.

tspan = (0.0, 2.0)
ode = semidiscretize(semi, tspan)

summary_callback = SummaryCallback()

analysis_interval = 100

analysis_callback = AnalysisCallback(semi, interval = analysis_interval)

alive_callback = AliveCallback(analysis_interval = analysis_interval)

save_solution = SaveSolutionCallback(interval = 100,
save_initial_solution = true,
save_final_solution = true,
solution_variables = cons2prim)

stepsize_callback = StepsizeCallback(cfl = 0.5)

callbacks = CallbackSet(summary_callback,
analysis_callback, alive_callback,
save_solution,
stepsize_callback)

###############################################################################
# run the simulation

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
68 changes: 68 additions & 0 deletions examples/tree_1d_dgsem/elixir_euler_quasi_1d_ec.jl
Original file line number Diff line number Diff line change
@@ -0,0 +1,68 @@
using OrdinaryDiffEq
using Trixi

###############################################################################
# Semidiscretization of the quasi 1d compressible Euler equations
# See Chan et al. https://doi.org/10.48550/arXiv.2307.12089 for details

equations = CompressibleEulerEquationsQuasi1D(1.4)

function initial_condition_ec(x, t, equations::CompressibleEulerEquationsQuasi1D)
v1 = 0.1
rho = 2.0 + 0.1 * x[1]
p = 3.0
a = 2.0 + x[1]

return prim2cons(SVector(rho, v1, p, a), equations)
end

initial_condition = initial_condition_ec

volume_flux = (flux_chan_etal, flux_nonconservative_chan_etal)
surface_flux = volume_flux
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basis = LobattoLegendreBasis(3)
solver = DGSEM(polydeg = 4, surface_flux = surface_flux,
volume_integral = VolumeIntegralFluxDifferencing(volume_flux))

coordinates_min = (-1.0,)
coordinates_max = (1.0,)
mesh = TreeMesh(coordinates_min, coordinates_max,
initial_refinement_level = 6,
n_cells_max = 10_000)

semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver)

###############################################################################
# ODE solvers, callbacks etc.

tspan = (0.0, 2.0)
ode = semidiscretize(semi, tspan)

summary_callback = SummaryCallback()

analysis_interval = 100

analysis_callback = AnalysisCallback(semi, interval = analysis_interval)

alive_callback = AliveCallback(analysis_interval = analysis_interval)

save_solution = SaveSolutionCallback(interval = 100,
save_initial_solution = true,
save_final_solution = true,
solution_variables = cons2prim)

stepsize_callback = StepsizeCallback(cfl = 0.5)

callbacks = CallbackSet(summary_callback,
analysis_callback, alive_callback,
save_solution,
stepsize_callback)

###############################################################################
# run the simulation

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
60 changes: 60 additions & 0 deletions examples/tree_1d_dgsem/elixir_euler_quasi_1d_source_terms.jl
Original file line number Diff line number Diff line change
@@ -0,0 +1,60 @@
using OrdinaryDiffEq
using Trixi
using ForwardDiff

###############################################################################
# Semidiscretization of the quasi 1d compressible Euler equations
# See Chan et al. https://doi.org/10.48550/arXiv.2307.12089 for details

equations = CompressibleEulerEquationsQuasi1D(1.4)

initial_condition = initial_condition_convergence_test

volume_flux = (flux_chan_etal, flux_nonconservative_chan_etal)
surface_flux = volume_flux
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solver = DGSEM(polydeg = 4, surface_flux = surface_flux,
volume_integral = VolumeIntegralFluxDifferencing(volume_flux))

coordinates_min = -1.0
coordinates_max = 1.0
mesh = TreeMesh(coordinates_min, coordinates_max,
initial_refinement_level = 4,
n_cells_max = 10_000)

semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver,
source_terms = source_terms_convergence_test)

###############################################################################
# ODE solvers, callbacks etc.

tspan = (0.0, 2.0)
ode = semidiscretize(semi, tspan)

summary_callback = SummaryCallback()

analysis_interval = 100
analysis_callback = AnalysisCallback(semi, interval = analysis_interval,
extra_analysis_errors = (:l2_error_primitive,
:linf_error_primitive))

alive_callback = AliveCallback(analysis_interval = analysis_interval)

save_solution = SaveSolutionCallback(interval = 100,
save_initial_solution = true,
save_final_solution = true,
solution_variables = cons2prim)

stepsize_callback = StepsizeCallback(cfl = 0.8)

callbacks = CallbackSet(summary_callback,
analysis_callback, alive_callback,
save_solution,
stepsize_callback)

###############################################################################
# run the simulation

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
1 change: 1 addition & 0 deletions src/Trixi.jl
Original file line number Diff line number Diff line change
Expand Up @@ -139,6 +139,7 @@ export AcousticPerturbationEquations2D,
CompressibleEulerEquations3D,
CompressibleEulerMulticomponentEquations1D,
CompressibleEulerMulticomponentEquations2D,
CompressibleEulerEquationsQuasi1D,
IdealGlmMhdEquations1D, IdealGlmMhdEquations2D, IdealGlmMhdEquations3D,
IdealGlmMhdMulticomponentEquations1D, IdealGlmMhdMulticomponentEquations2D,
HyperbolicDiffusionEquations1D, HyperbolicDiffusionEquations2D,
Expand Down
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