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98 changes: 98 additions & 0 deletions
98
examples/p4est_2d_dgsem/elixir_advection_diffusion_nonperiodic_amr.jl
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the linear advection-diffusion equation | ||
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diffusivity() = 5.0e-2 | ||
advection_velocity = (1.0, 0.0) | ||
equations = LinearScalarAdvectionEquation2D(advection_velocity) | ||
equations_parabolic = LaplaceDiffusion2D(diffusivity(), equations) | ||
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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, -0.5) # minimum coordinates (min(x), min(y)) | ||
coordinates_max = (0.0, 0.5) # maximum coordinates (max(x), max(y)) | ||
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trees_per_dimension = (4, 4) | ||
mesh = P4estMesh(trees_per_dimension, | ||
polydeg = 3, initial_refinement_level = 2, | ||
coordinates_min = coordinates_min, coordinates_max = coordinates_max, | ||
periodicity = false) | ||
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# Example setup taken from | ||
# - Truman Ellis, Jesse Chan, and Leszek Demkowicz (2016). | ||
# Robust DPG methods for transient convection-diffusion. | ||
# In: Building bridges: connections and challenges in modern approaches | ||
# to numerical partial differential equations. | ||
# [DOI](https://doi.org/10.1007/978-3-319-41640-3_6). | ||
function initial_condition_eriksson_johnson(x, t, equations) | ||
l = 4 | ||
epsilon = diffusivity() # TODO: this requires epsilon < .6 due to sqrt | ||
lambda_1 = (-1 + sqrt(1 - 4 * epsilon * l)) / (-2 * epsilon) | ||
lambda_2 = (-1 - sqrt(1 - 4 * epsilon * l)) / (-2 * epsilon) | ||
r1 = (1 + sqrt(1 + 4 * pi^2 * epsilon^2)) / (2 * epsilon) | ||
s1 = (1 - sqrt(1 + 4 * pi^2 * epsilon^2)) / (2 * epsilon) | ||
u = exp(-l * t) * (exp(lambda_1 * x[1]) - exp(lambda_2 * x[1])) + | ||
cos(pi * x[2]) * (exp(s1 * x[1]) - exp(r1 * x[1])) / (exp(-s1) - exp(-r1)) | ||
return SVector{1}(u) | ||
end | ||
initial_condition = initial_condition_eriksson_johnson | ||
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boundary_conditions = Dict(:x_neg => BoundaryConditionDirichlet(initial_condition), | ||
:y_neg => BoundaryConditionDirichlet(initial_condition), | ||
:y_pos => BoundaryConditionDirichlet(initial_condition), | ||
:x_pos => boundary_condition_do_nothing) | ||
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boundary_conditions_parabolic = Dict(:x_neg => BoundaryConditionDirichlet(initial_condition), | ||
:x_pos => BoundaryConditionDirichlet(initial_condition), | ||
:y_neg => BoundaryConditionDirichlet(initial_condition), | ||
:y_pos => BoundaryConditionDirichlet(initial_condition)) | ||
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# A semidiscretization collects data structures and functions for the spatial discretization | ||
semi = SemidiscretizationHyperbolicParabolic(mesh, | ||
(equations, equations_parabolic), | ||
initial_condition, solver; | ||
boundary_conditions = (boundary_conditions, | ||
boundary_conditions_parabolic)) | ||
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############################################################################### | ||
# ODE solvers, callbacks etc. | ||
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# Create ODE problem with time span `tspan` | ||
tspan = (0.0, 0.5) | ||
ode = semidiscretize(semi, tspan) | ||
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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_interval = 1000 | ||
analysis_callback = AnalysisCallback(semi, interval = analysis_interval) | ||
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# The AliveCallback prints short status information in regular intervals | ||
alive_callback = AliveCallback(analysis_interval = analysis_interval) | ||
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amr_controller = ControllerThreeLevel(semi, IndicatorMax(semi, variable = first), | ||
base_level = 1, | ||
med_level = 2, med_threshold = 0.9, | ||
max_level = 3, max_threshold = 1.0) | ||
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amr_callback = AMRCallback(semi, amr_controller, | ||
interval = 50) | ||
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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, alive_callback, amr_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 | ||
time_int_tol = 1.0e-11 | ||
sol = solve(ode, dt = 1e-7, RDPK3SpFSAL49(); abstol = time_int_tol, reltol = time_int_tol, | ||
ode_default_options()..., callback = callbacks) | ||
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# Print the timer summary | ||
summary_callback() |
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examples/p4est_2d_dgsem/elixir_advection_diffusion_periodic_amr.jl
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using OrdinaryDiffEq | ||
using Trixi | ||
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############################################################################### | ||
# semidiscretization of the linear advection-diffusion equation | ||
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advection_velocity = (1.5, 1.0) | ||
equations = LinearScalarAdvectionEquation2D(advection_velocity) | ||
diffusivity() = 5.0e-2 | ||
equations_parabolic = LaplaceDiffusion2D(diffusivity(), equations) | ||
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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) # minimum coordinates (min(x), min(y)) | ||
coordinates_max = (1.0, 1.0) # maximum coordinates (max(x), max(y)) | ||
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trees_per_dimension = (4, 4) | ||
mesh = P4estMesh(trees_per_dimension, | ||
polydeg = 3, initial_refinement_level = 1, | ||
coordinates_min = coordinates_min, coordinates_max = coordinates_max) | ||
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# Define initial condition | ||
function initial_condition_diffusive_convergence_test(x, t, | ||
equation::LinearScalarAdvectionEquation2D) | ||
# Store translated coordinate for easy use of exact solution | ||
x_trans = x - equation.advection_velocity * t | ||
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nu = diffusivity() | ||
c = 1.0 | ||
A = 0.5 | ||
L = 2 | ||
f = 1 / L | ||
omega = 2 * pi * f | ||
scalar = c + A * sin(omega * sum(x_trans)) * exp(-2 * nu * omega^2 * t) | ||
return SVector(scalar) | ||
end | ||
initial_condition = initial_condition_diffusive_convergence_test | ||
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# A semidiscretization collects data structures and functions for the spatial discretization | ||
semi = SemidiscretizationHyperbolicParabolic(mesh, | ||
(equations, equations_parabolic), | ||
initial_condition, solver) | ||
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############################################################################### | ||
# ODE solvers, callbacks etc. | ||
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# Create ODE problem with time span `tspan` | ||
tspan = (0.0, 0.5) | ||
ode = semidiscretize(semi, tspan); | ||
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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_interval = 100 | ||
analysis_callback = AnalysisCallback(semi, interval = analysis_interval) | ||
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# The AliveCallback prints short status information in regular intervals | ||
alive_callback = AliveCallback(analysis_interval = analysis_interval) | ||
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amr_controller = ControllerThreeLevel(semi, IndicatorMax(semi, variable = first), | ||
base_level = 1, | ||
med_level = 2, med_threshold = 1.25, | ||
max_level = 3, max_threshold = 1.45) | ||
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amr_callback = AMRCallback(semi, amr_controller, | ||
interval = 20) | ||
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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, alive_callback, amr_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 | ||
time_int_tol = 1.0e-11 | ||
sol = solve(ode, RDPK3SpFSAL49(); abstol = time_int_tol, reltol = time_int_tol, | ||
ode_default_options()..., callback = callbacks) | ||
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# Print the timer summary | ||
summary_callback() |
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