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Nonsingular kernel boundary integral and finite element coupling method

机译:非奇异核边界积分与有限元耦合方法

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In the finite element and boundary element coupling method, the Stekhlov-Poincare mapping is often adopted at the coupling boundary, i.e., the unknown Neumann data are represented by the unknown Dirichlet data on the same boundary. This coupling method (either by a convolution integral, or by a Fourier series) is referred as the conventional method. We propose an alternative method, where the unknown Dirichlet data at the boundary are represented by the unknown solution value on an interior curve or surface, i.e., a Dirichlet-to-Dirichlet (D-to-D) mapping is employed instead of a Dirichletto-Neumann (D-to-N) mapping. The convergence of the method is shown to be of optimal order. 2D and 3D numerical experiments are performed to demonstrate the accuracy of the proposed method, comparing to the two conventional D-to-N coupling methods. (C) 2018 IMACS. Published by Elsevier B.V. All rights reserved.
机译:在有限元和边界元耦合方法中,通常在耦合边界处采用Stekhlov-Poincare映射,即未知Neumann数据由同一边界上的未知Dirichlet数据表示。该耦合方法(通过卷积积分或傅里叶级数)被称为常规方法。我们提出了一种替代方法,其中边界处的未知Dirichlet数据由内部曲线或曲面上的未知解值表示,即采用Dirichlet到Dirichlet(D到D)映射代替Dirichletto -Neumann(D到N)映射。该方法的收敛被证明是最优阶的。与两种传统的D-N耦合方法相比,进行了2D和3D数值实验以证明所提出方法的准确性。 (C)2018年IMACS。由Elsevier B.V.发布。保留所有权利。

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