Adding quasi 1d shallow water equations

examples/tree_1d_dgsem/elixir_shallow_water_quasi_1d_source_terms.jl

@@ -0,0 +1,60 @@
+using OrdinaryDiffEq
+using Trixi
+
+###############################################################################
+# Semidiscretization of the quasi 1d shallow water equations
+# See Chan et al.  https://doi.org/10.48550/arXiv.2307.12089 for details
+
+equations = ShallowWaterEquationsQuasi1D(gravity_constant = 9.81)
+
+initial_condition = initial_condition_convergence_test
+
+###############################################################################
+# Get the DG approximation space
+
+volume_flux = (flux_chan_etal, flux_nonconservative_chan_etal)
+surface_flux = (FluxPlusDissipation(flux_chan_etal, DissipationLocalLaxFriedrichs()),
+                flux_nonconservative_chan_etal)
+solver = DGSEM(polydeg = 3, surface_flux = surface_flux,
+               volume_integral = VolumeIntegralFluxDifferencing(volume_flux))
+
+###############################################################################
+# Get the TreeMesh and setup a periodic mesh
+
+coordinates_min = 0.0
+coordinates_max = sqrt(2.0)
+mesh = TreeMesh(coordinates_min, coordinates_max,
+                initial_refinement_level = 3,
+                n_cells_max = 10_000,
+                periodicity = true)
+
+# create the semi discretization object
+semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver,
+                                    source_terms = source_terms_convergence_test)
+
+###############################################################################
+# ODE solvers, callbacks etc.
+
+tspan = (0.0, 1.0)
+ode = semidiscretize(semi, tspan)
+
+summary_callback = SummaryCallback()
+
+analysis_interval = 500
+analysis_callback = AnalysisCallback(semi, interval = analysis_interval)
+
+alive_callback = AliveCallback(analysis_interval = analysis_interval)
+
+save_solution = SaveSolutionCallback(interval = 200,
+                                     save_initial_solution = true,
+                                     save_final_solution = true)
+
+callbacks = CallbackSet(summary_callback, analysis_callback, alive_callback, save_solution)
+
+###############################################################################
+# run the simulation
+
+# use a Runge-Kutta method with automatic (error based) time step size control
+sol = solve(ode, RDPK3SpFSAL49(); abstol = 1.0e-8, reltol = 1.0e-8,
+            ode_default_options()..., callback = callbacks);
+summary_callback() # print the timer summary

examples/tree_1d_dgsem/elixir_shallowwater_quasi_1d_well_balanced.jl

@@ -0,0 +1,84 @@
+using OrdinaryDiffEq
+using Trixi
+
+###############################################################################
+# semidiscretization of the shallow water equations with a discontinuous
+# bottom topography function and channel width function
+
+equations = ShallowWaterEquationsQuasi1D(gravity_constant = 9.81, H0 = 2.0)
+
+# Setup a truly discontinuous bottom topography function and channel width for
+# this academic testcase of well-balancedness. The errors from the analysis
+# callback are not important but the error for this lake-at-rest test case
+# `∑|H0-(h+b)|` should be around machine roundoff.
+# Works as intended for TreeMesh1D with `initial_refinement_level=3`. If the mesh
+# refinement level is changed the initial condition below may need changed as well to
+# ensure that the discontinuities lie on an element interface.
+function initial_condition_discontinuous_well_balancedness(x, t,
+                                                           equations::ShallowWaterEquationsQuasi1D)
+    H = equations.H0
+    v = 0.0
+
+    # for a periodic domain, this choice of `b` and `a` mimic 
+    # discontinuity across the periodic boundary.
+    b = 0.5 * (x[1] + 1)
+    a = 2 + x[1]
+
+    return prim2cons(SVector(H, v, b, a), equations)
+end
+
+initial_condition = initial_condition_discontinuous_well_balancedness
+
+###############################################################################
+# Get the DG approximation space
+
+volume_flux = (flux_chan_etal, flux_nonconservative_chan_etal)
+surface_flux = volume_flux
+solver = DGSEM(polydeg = 4, surface_flux = surface_flux,
+               volume_integral = VolumeIntegralFluxDifferencing(volume_flux))
+
+###############################################################################
+# Get the TreeMesh and setup a periodic mesh
+
+coordinates_min = -1.0
+coordinates_max = 1.0
+mesh = TreeMesh(coordinates_min, coordinates_max,
+                initial_refinement_level = 3,
+                n_cells_max = 10_000)
+
+# Create the semi discretization object
+semi = SemidiscretizationHyperbolic(mesh, equations, initial_condition, solver)
+
+###############################################################################
+# ODE solver
+
+tspan = (0.0, 100.0)
+ode = semidiscretize(semi, tspan)
+
+###############################################################################
+# Callbacks
+
+summary_callback = SummaryCallback()
+
+analysis_interval = 1000
+analysis_callback = AnalysisCallback(semi, interval = analysis_interval,
+                                     extra_analysis_integrals = (lake_at_rest_error,))
+
+alive_callback = AliveCallback(analysis_interval = analysis_interval)
+
+save_solution = SaveSolutionCallback(interval = 1000,
+                                     save_initial_solution = true,
+                                     save_final_solution = true)
+
+stepsize_callback = StepsizeCallback(cfl = 3.0)
+
+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

src/Trixi.jl

@@ -149,6 +149,7 @@ export AcousticPerturbationEquations2D,
        LatticeBoltzmannEquations2D, LatticeBoltzmannEquations3D,
        ShallowWaterEquations1D, ShallowWaterEquations2D,
        ShallowWaterTwoLayerEquations1D, ShallowWaterTwoLayerEquations2D,
+       ShallowWaterEquationsQuasi1D,
        LinearizedEulerEquations2D
 
 export LaplaceDiffusion1D, LaplaceDiffusion2D,
@@ -164,6 +165,7 @@ export flux, flux_central, flux_lax_friedrichs, flux_hll, flux_hllc, flux_hlle,
        flux_kennedy_gruber, flux_shima_etal, flux_ec,
        flux_fjordholm_etal, flux_nonconservative_fjordholm_etal, flux_es_fjordholm_etal,
        flux_wintermeyer_etal, flux_nonconservative_wintermeyer_etal,
+       flux_chan_etal, flux_nonconservative_chan_etal,
        hydrostatic_reconstruction_audusse_etal, flux_nonconservative_audusse_etal,
 # TODO: TrixiShallowWater: move anything with "chen_noelle" to new file
        hydrostatic_reconstruction_chen_noelle, flux_nonconservative_chen_noelle,

src/equations/equations.jl

@@ -356,6 +356,7 @@ include("shallow_water_1d.jl")
 include("shallow_water_2d.jl")
 include("shallow_water_two_layer_1d.jl")
 include("shallow_water_two_layer_2d.jl")
+include("shallow_water_quasi_1d.jl")
 
 # CompressibleEulerEquations
 abstract type AbstractCompressibleEulerEquations{NDIMS, NVARS} <: