9: Other SBP schemes (FD, CGSEM) via DGMulti
solver
For a tutorial about DG schemes via the DGMulti
solver please visit the previous tutorial. The DGMulti
solver also supports other methods than DG. The important property a method has to fulfill is the summation-by-parts (SBP) property. The package SummationByPartsOperators.jl provides such methods, like a finite difference SBP (FD SBP) scheme. To do this, you need to create an SBP derivative operator and pass that as approximation_type
to the DGMulti
constructor. For example, the classical second-order FD SBP operator can be created as
using Trixi.SummationByPartsOperators # or add SummationByPartsOperators to your project and use it directly
D = derivative_operator(MattssonNordström2004(), derivative_order = 1, accuracy_order = 2,
xmin = 0.0, xmax = 1.0, N = 11)
SBP first-derivative operator of order 2 on a grid in [0.0, 1.0] using 11 nodes
and coefficients of Mattsson, Nordström (2004)
Summation by parts operators for finite difference approximations of second
derivatives.
Journal of Computational Physics 199, pp. 503-540.
Here, the arguments xmin
and xmax
do not matter beyond setting the real type used for the operator - they just set a reference element and are rescaled on the physical elements. The parameter N
determines the number of finite difference nodes. Then, D
can be used as approximation_type
like SBP()
in a multi-block fashion. In multiple dimensions, such a 1D SBP operator will be used in a tensor product fashion, i.e., in each coordinate direction. In particular, you can use them only on 1D, 2D Quad()
, and 3D Hex()
elements.
You can also use fully periodic single-block FD methods by creating a periodic SBP operator. For example, a fully periodic FD operator can be constructed as
D = periodic_derivative_operator(derivative_order = 1, accuracy_order = 2,
xmin = 0.0, xmax = 1.0, N = 11)
Periodic first-derivative operator of order 2 on a grid in [0.0, 1.0] using 11 nodes,
stencils with 1 nodes to the left, 1 nodes to the right, and coefficients of Fornberg (1998)
Calculation of Weights in Finite Difference Formulas.
SIAM Rev. 40.3, pp. 685-691.
An example using such an FD method is implemented in elixir_euler_fdsbp_periodic.jl
. For all parameters and other calling options, please have a look in the documentation of SummationByPartsOperators.jl.
Another possible method is for instance a continuous Galerkin (CGSEM) method. You can use such a method with polynomial degree of 3
(N=4
Legendre Lobatto nodes on [0, 1]
) coupled continuously on a uniform mesh with Nx=10
elements by setting approximation_type
to
using Trixi.SummationByPartsOperators # or add SummationByPartsOperators to your project and use it directly
D = couple_continuously(legendre_derivative_operator(xmin = 0.0, xmax = 1.0, N = 4),
UniformPeriodicMesh1D(xmin = -1.0, xmax = 1.0, Nx = 10))
First derivative operator {T=Float64} on 4 Lobatto Legendre nodes in [0.0, 1.0]
coupled continuously on SummationByPartsOperators.UniformPeriodicMesh1D{Float64} with 10 cells in (-1.0, 1.0)
To choose a discontinuous coupling (DGSEM), use couple_discontinuously()
instead of couple_continuously()
.
For more information and other SBP operators, see the documentations of StartUpDG.jl and SummationByPartsOperators.jl.
Package versions
These results were obtained using the following versions.
using InteractiveUtils
versioninfo()
using Pkg
Pkg.status(["Trixi", "StartUpDG", "SummationByPartsOperators"],
mode = PKGMODE_MANIFEST)
Julia Version 1.10.7
Commit 4976d05258e (2024-11-26 15:57 UTC)
Build Info:
Official https://julialang.org/ release
Platform Info:
OS: Linux (x86_64-linux-gnu)
CPU: 4 × AMD EPYC 7763 64-Core Processor
WORD_SIZE: 64
LIBM: libopenlibm
LLVM: libLLVM-15.0.7 (ORCJIT, znver3)
Threads: 1 default, 0 interactive, 1 GC (on 4 virtual cores)
Environment:
JULIA_PKG_SERVER_REGISTRY_PREFERENCE = eager
Status `~/work/Trixi.jl/Trixi.jl/docs/Manifest.toml`
[472ebc20] StartUpDG v1.1.5
[9f78cca6] SummationByPartsOperators v0.5.72
[a7f1ee26] Trixi v0.9.12 `~/work/Trixi.jl/Trixi.jl`
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