2008
DOI: 10.1111/j.1365-246x.2008.03915.x
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The interior penalty discontinuous Galerkin method for elastic wave propagation: grid dispersion

Abstract: S U M M A R YRecently, there has been an increased interest in applying the discontinuous Galerkin method (DGM) to wave propagation. In this work, we investigate the applicability of the interior penalty DGM to elastic wave propagation by analysing it's grid dispersion properties, with particular attention to the effect that different basis functions have on the numerical dispersion. We consider different types of basis functions that naturally yield a diagonal mass matrix. This is relevant to seismology becau… Show more

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Cited by 155 publications
(95 citation statements)
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References 34 publications
(74 reference statements)
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“…Rational functions [34] or sines and cosines [35] can also be considered as basis functions. Discontinuous Galerkin methods [36][37][38] allow for the use of standard high-order elements. Since the mass matrix is local, it is readily inverted.…”
Section: Discussionmentioning
confidence: 99%
“…Rational functions [34] or sines and cosines [35] can also be considered as basis functions. Discontinuous Galerkin methods [36][37][38] allow for the use of standard high-order elements. Since the mass matrix is local, it is readily inverted.…”
Section: Discussionmentioning
confidence: 99%
“…Let us quote few examples: Ainsworth et al (2006) provided a theoretical study for the 1D case; Basabe et al (2008) analysed the effects of basis functions on 2D periodic and regular quadrilateral meshes; and discussed the convergence of the DG-FEM combined with ADER time integration and 3D tetrahedral meshes. More related to our particular concern here, Delcourte et al (2009) provided a convergence analysis of the DG-FEM with a centred flux scheme and tetrahedral meshes for elastodynamics.…”
Section: Accuracy Of Dg-fem With Tetrahedral Meshesmentioning
confidence: 99%
“…More specifically, the numerical algorithm can be summarized in the following steps ( Fig. 10.3): consider an elastic heterogeneous 3D medium, (i) make a partition of the computational domain based on the involved materials and/or structures to be simulated, (ii) select a suitable spectral-element discretization in each non-overlapping sub-region, and (iii) enforce the continuity of the numerical solution at the internal interfaces by treating the jumps of the displacements through a suitable DG algorithm of the interior penalty type (De Basabe et al 2008).…”
Section: Development Of the Numerical Codementioning
confidence: 99%