2018
DOI: 10.4208/jcm.1610-m2015-0480
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A BIE-Based DtN-FEM for Fluid-Solid Interaction Problems

Abstract: In this paper, we are concerned with the coupling of finite element methods and boundary integral equation methods solving the classical fluid-solid interaction problem in two dimensions. The original transmission problem is reduced to an equivalent nonlocal boundary value problem via introducing a Dirichlet-to-Neumann mapping by the direct boundary integral equation method. We show the existence and uniqueness of the solution for the corresponding variational equation. Numerical results based on the finite el… Show more

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Cited by 9 publications
(3 citation statements)
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“…One popular method to overcome the difficulty that the acoustic scattered wave propagates in an unbounded domain is known as the Dirichlet-to-Neumann (DtN) method ( [9,28,29]), that is, the original transmission problem is reduced to a boundary value problem by introducing a DtN mapping defined on an artificial boundary enclosing the elastic body inside. Another conventional numerical method is the coupling of the boundary element method (BEM) and the finite element method (FEM) ( [7,8,[10][11][12][13][14]24]).…”
Section: Introductionmentioning
confidence: 99%
“…One popular method to overcome the difficulty that the acoustic scattered wave propagates in an unbounded domain is known as the Dirichlet-to-Neumann (DtN) method ( [9,28,29]), that is, the original transmission problem is reduced to a boundary value problem by introducing a DtN mapping defined on an artificial boundary enclosing the elastic body inside. Another conventional numerical method is the coupling of the boundary element method (BEM) and the finite element method (FEM) ( [7,8,[10][11][12][13][14]24]).…”
Section: Introductionmentioning
confidence: 99%
“…We consider the scattering of a plane incident wave p inc = e ikx•d with direction d = (1, 0) by a disc-shaped elastic body of radius R 0 (see Figure 2). For the exact solution of this model problem, we refer to [28,39]. In numerical computations, the computational domain Ω and Ω R are discretized by uniform triangle elements and we employ piecewise linear basis functions {ϕ i } i=N1 i=1 and {ψ i } i=N2 i=1 in Ω and Ω R , respectively, to construct the finite element space H h .…”
Section: Numerical Experimentsmentioning
confidence: 99%
“…Some of them provide proper guidance also for time-domain problems. Popular methods include the boundary integral equation (BIE) method, see [33,46] and coupling methods such as the so-called coupled FEM-BEM method, see [47]. An artificial boundary or an absorbing layer ( [43]) can be introduced to reduce the original unbounded problem to a bounded problem which could be solved using field equation solvers such as the finite element method.…”
Section: Introductionmentioning
confidence: 99%