2000
DOI: 10.1007/978-3-642-59721-3_15
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Explicit Finite Element Methods for Linear Hyperbolic Systems

Abstract: Abstract. Our focus is on explicit £nite element discretization of transient, linear hyperbolic systems in arbitrarily many space dimensions. We propose several ways of generating suitable "explicit" meshes, and sketch an O(h n+1/2 ) error estimate for a discontinuous Galerkin method. Continuous methods are also considered brie¤y. This paper parallels [2] in large part, while using a different approach in the analysis.

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Cited by 6 publications
(6 citation statements)
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“…An innovative implicit space–time DGM with basis functions that are free‐space solutions of the PDE governing the problem of interest was proposed in for the solution of wave propagation problems in the time domain. By partitioning the space–time domain carefully, systems of equations, which are independent of each other, can be formulated on clusters of neighboring elements, independently of other such clusters, yielding a semi‐implicit method .…”
Section: Introductionmentioning
confidence: 99%
“…An innovative implicit space–time DGM with basis functions that are free‐space solutions of the PDE governing the problem of interest was proposed in for the solution of wave propagation problems in the time domain. By partitioning the space–time domain carefully, systems of equations, which are independent of each other, can be formulated on clusters of neighboring elements, independently of other such clusters, yielding a semi‐implicit method .…”
Section: Introductionmentioning
confidence: 99%
“…Various DG methods can be applied to solve linear hyperbolic systems. We mention the classical Runge-Kutta DG method of Cockburn and Shu [10], the nodal DG method of Hesthaven and Warburton [16], the space-time DG method of Falk and Richter [12] and Monk and Richter [23]. All these DG methods use approximate/exact Riemann solvers to define the numerical flux, and are dissipative by design.…”
Section: Introductionmentioning
confidence: 99%
“…12: long time simulation: advection of a Gaussian pulse. We consider the advection equation (4.2) on the unit square with periodic boundary condition and initial condition u(x, y, 0) = exp(−200((x − 0.5) 2 + (y − .5) 2 )).…”
mentioning
confidence: 99%
“…Recently, new explicit finite element methods with unstructured meshes based on the discontinuous Galerkin method are suggested for elastodynamics problems [16,17,18]. The methods allow an element-by-element solution in a space-time domain.…”
Section: Introductionmentioning
confidence: 99%