2003
DOI: 10.1007/s00211-002-0447-4
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A Conservative Space-time Mesh Refinement Method for the 1-D Wave Equation. Part II: Analysis

Abstract: We introduced in [2] a new method for space-time refinement for the 1-D wave equation. This method is based on the conservation of a discrete energy through two different discretization grids which guarantees the stability of the scheme. In this second part, we analyse the accuracy of this scheme in a detailed way by means of a plane wave analysis and numerical experiments that permit us to point out spurious numerical phenomena and explain how to control them.

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Cited by 50 publications
(50 citation statements)
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“…Our construction of a stable time discretization of the continuous equations will be based on this conservation property (as for instance in the work of [13], [15], [3]). …”
Section: Energy and A Priori Estimatesmentioning
confidence: 99%
“…Our construction of a stable time discretization of the continuous equations will be based on this conservation property (as for instance in the work of [13], [15], [3]). …”
Section: Energy and A Priori Estimatesmentioning
confidence: 99%
“…Highly e cient in practice, centered time discretizations also display remarkably high accuracy over long times and remain even nowadays probably the most popular methods for the time integration of wave equations. In [13] Collino, Fouquet and Joly proposed an LTS method for the wave equation in first-order form, which conserves a discrete energy yet requires every time-step the solution of a linear system on the interface between the coarse and the fine mesh. It was analyzed in [14,15] and later extended to elastodynamics [16] and Maxwell's equations [17].…”
Section: Introductionmentioning
confidence: 99%
“…In [13] Collino, Fouquet and Joly proposed an LTS method for the wave equation in first-order form, which conserves a discrete energy yet requires every time-step the solution of a linear system on the interface between the coarse and the fine mesh. It was analyzed in [14,15] and later extended to elastodynamics [16] and Maxwell's equations [17]. By combining a symplectic integrator with a DG discretization of Maxwell's equations in first-order form, Piperno [18] proposed a second-order explicit local time-stepping scheme, which also conserves a discrete energy.…”
Section: Introductionmentioning
confidence: 99%
“…To overcome the overly restrictive stability constraint, various LTS schemes (Collino et al, 2003;Piperno, 2006) have been developed, which use either implicit time-stepping or explicit but smaller time steps, but only where the smallest elements in the mesh are located. Because DGMs allow for a local formulation, they are particularly well suited for the development of explicit LTS schemes.…”
Section: Introductionmentioning
confidence: 99%