2017
DOI: 10.1093/gji/ggx470
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On long-time instabilities in staggered finite difference simulations of the seismic acoustic wave equations on discontinuous grids

Abstract: SUMMARYWe consider the long-time instability issue associated with finite difference simulation of seismic acoustic wave equations on discontinuous grids. This issue is exhibited by a prototype algebraic problem abstracted from practical application settings.Analysis of this algebraic problem leads to better understanding of the cause of the instability and provides guidance for its treatment. Specifically, we use the concept of discrete energy to derive the proper solution transfer operators and design an eff… Show more

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Cited by 4 publications
(10 citation statements)
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“…such that the wave can pass through the interface smoothly without interference. In this section, we explain how to impose the interface conditions in (18) with the SATs. In order to focus on the interface treatment, we assume that both boundaries (x L and x R ) have been satisfactorily dealt with by some SBP discretization operators and SATs in an energy-conserving manner so that in the upcoming energy analysis, no term pops out in Q due to the boundaries.…”
Section: Imposing Interface Conditions For the 1d Model Problemmentioning
confidence: 99%
“…such that the wave can pass through the interface smoothly without interference. In this section, we explain how to impose the interface conditions in (18) with the SATs. In order to focus on the interface treatment, we assume that both boundaries (x L and x R ) have been satisfactorily dealt with by some SBP discretization operators and SATs in an energy-conserving manner so that in the upcoming energy analysis, no term pops out in Q due to the boundaries.…”
Section: Imposing Interface Conditions For the 1d Model Problemmentioning
confidence: 99%
“…Left multiplying (42) with ḃT and recalling the definitions of the discrete energies in (20), we have the following result:…”
Section: Interface Treatmentmentioning
confidence: 99%
“…regarding the discrete energy associated with (42) in the FEM region. When it comes to implementation, the line integral ∂I in ( 43) is usually replaced by quadrature.…”
Section: Interface Treatmentmentioning
confidence: 99%
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