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Stable least-squares space-time boundary element methods for the wave equation
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abstract
In this paper, we recast the variational formulation corresponding to the single layer boundary integral operator $\operatorname{V}$ for the wave equation as a minimization problem in $L^2(\Sigma)$, where $\Sigma := \partial \Omega \times (0,T)$ is the lateral boundary of the space-time domain $Q := \Omega \times (0,T)$. For discretization, the minimization problem is restated as a mixed saddle point formulation. Unique solvability is established by combining conforming nested boundary element spaces for the mixed formulation such that the related bilinear form is discrete inf-sup stable. We analyze under which conditions the discrete inf-sup stability is satisfied, and, moreover, we show that the mixed formulation provides a simple error indicator, which can be used for adaptivity. We present several numerical experiments showing the applicability of the method to different time-domain boundary integral formulations used in the literature.
Forward citations
Cited by 2 Pith papers
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A space-time adaptive boundary element method for the wave equation
A space-time adaptive boundary element method with residual error indicators is shown numerically to achieve roughly twice the convergence rate of uniform refinement for 2D wave scattering with singularities.
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Paving the way to a $\operatorname{T}$-coercive method for the wave equation
A parameter-dependent transformation T_mu makes the weak form of u''+mu u=f coercive with mu-independent stability, a step toward a T-coercive space-time wave equation method.
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