2017
DOI: 10.1016/j.jcp.2017.07.032
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An accurate boundary element method for the exterior elastic scattering problem in two dimensions

Abstract: This paper is concerned with a Galerkin boundary element method solving the two dimensional exterior elastic wave scattering problem. The original problem is first reduced to the so-called ) boundary integral formulation, and essential mathematical features of its variational form are discussed.In numerical implementations, a newly-derived and analytically accurate regularization formula ([18]

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Cited by 30 publications
(21 citation statements)
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“…In this section, we derive an accurate regularized formulation for the hypersingular boundary integral operator N˜w in light of the techniques presented in References 28,29 for the closed‐surface case. The regularized formulation for the hypersingular boundary integral operator N w can be obtained directly by letting μ˜=μ.…”
Section: Weighted Operators and New Integral Solversmentioning
confidence: 99%
See 1 more Smart Citation
“…In this section, we derive an accurate regularized formulation for the hypersingular boundary integral operator N˜w in light of the techniques presented in References 28,29 for the closed‐surface case. The regularized formulation for the hypersingular boundary integral operator N w can be obtained directly by letting μ˜=μ.…”
Section: Weighted Operators and New Integral Solversmentioning
confidence: 99%
“…A number of additional techniques are proposed to accurately evaluate the elastic hypersingular integral operators N w and N˜w. For closed‐surface scattering problems in elasticity, the novel and exact regularized formulation presented in References 28,29 show that the hypersingular operator in two dimensions can be transformed into a composition of weakly singular integrals and tangential‐derivative operators that involve the Günter derivative and integration‐by‐parts. For the weighted hypersingular operators N w and N˜w in the open‐arc case, thanks to the edge‐vanishing weight function w , the results in the closed‐surface case can be extended to the open‐arc case since all singular terms arising from the integration‐by‐parts calculation can be eliminated.…”
Section: Introductionmentioning
confidence: 99%
“…As one of the most fundamental numerical methods, the boundary integral equation (BIE) method [25] has been extensively developed for numerical solutions of partial differential equations problems with various structures including bounded closed-surface [4,8,12], open screens [9][10][11]27,35], period or non-period infinite surface [13], and so on. The BIE method has a feature of discretization of domains with lower dimensionality, and it is also a feasible method for the numerics of high frequency scattering problems.…”
Section: Introductionmentioning
confidence: 99%
“…One usually needs additional treatments in numerics for the correct evaluation of the classically non-integrable boundary integrals arising from the hyper-singular BIO. There are already existing many works ( [2,15,16,19,26,27,29,30,38]) on this issue, and the main idea consists of rewriting the hyper-singular BIO in terms of a composition of differentiation and weakly singular operators for the Laplace equation, the Helmholtz equation, the time-harmonic Navier equation and the Lamé equation. This composition, in fact, is a regularization procedure ( [19,38]) of the hyper-singular distribution, and is useful for the variational formulation and related computational procedures.…”
Section: Introductionmentioning
confidence: 99%
“…For each problem, we apply the double-layer potential to represent the solution, and then the original boundary value problem is reduced to a Fredholm boundary integral equation of the first kind with the corresponding hyper-singular BIO. Following the work in [2,38] for the two-dimensional case, and utilizing the tangential Günter derivative, we derive the new and analytically accurate regularized formulations for the hyper-singular BIO associated with the three dimensional timeharmonic Navier equation and Biot system of linearized thermoelasticity, respectively. As a result, in the corresponding weak forms, all involved integrals are at most weakly-singular.…”
Section: Introductionmentioning
confidence: 99%