Abstract
Different time-stepping methods for a nodal high-order discontinuous Galerkin discretisation of the Maxwell equations are discussed. A comparison between the most popular choices of Runge-Kutta (RK) methods is made from the point of view of accuracy and computational work. By choosing the strong-stability-preserving Runge-Kutta (SSP-RK) time-integration method of order consistent with the polynomial order of the spatial discretisation, better accuracy can be attained compared with fixed-order schemes. Moreover, this comes without a significant increase in the computational work. A numerical Fourier analysis is performed for this Runge-Kutta discontinuous Galerkin (RKDG) discretisation to gain insight into the dispersion and dissipation properties of the fully discrete scheme. The analysis is carried out on both the one-dimensional and the two-dimensional fully discrete schemes and, in the latter case, on uniform as well as on non-uniform meshes. It also provides practical information on the convergence of the dissipation and dispersion error up to polynomial order 10 for the one-dimensional fully discrete scheme.
| Original language | Undefined |
|---|---|
| Pages (from-to) | 47-74 |
| Number of pages | 35 |
| Journal | Journal of scientific computing |
| Volume | 33 |
| Issue number | LNCS4549/1 |
| DOIs | |
| Publication status | Published - Jul 2007 |
Keywords
- Maxwell equations
- High-order nodal discontinuous Galerkin methods · Maxwell equations · Numerical dispersion and dissipation · Strong-stability-preserving Runge-Kutta methods
- EWI-10903
- high-order nodal discontinuous Galerkin methods
- numerical dispersion and dissipation strong-stability-preserving Runge-Kutta methods
- MSC-65L06
- MSC-65M20
- MSC-65M60
- METIS-241848
- IR-64298
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