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arXiv 2210.02432math.NAcs.NAmath.AP
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Lipschitz 域上 Laplace Dirichlet 问题的强制第二类边界积分方程

Coercive second-kind boundary integral equations for the Laplace Dirichlet problem on Lipschitz domains

Simon N. Chandler-Wilde, Euan A. Spence

AI总结:

针对Lipschitz域上Laplace Dirichlet问题,提出连续且强制的第二类边界积分方程新公式,确保Galerkin方法收敛且矩阵良态,克服了标准公式在某些域上不收敛的缺陷。

摘要:

我们提出了 Laplace 方程内部和外部 Dirichlet 问题的新第二类积分方程公式。这些公式中的算子均在 $\mathbb{R}^d$($d\geq 2$)中的一般 Lipschitz 域上的空间 $L^2(\Gamma)$ 中连续且强制,其中 $\Gamma$ 表示域的边界。连续性和强制性的这些性质立即意味着:(i)Galerkin 方法应用于这些公式时收敛;(ii)随着离散化细化,Galerkin 矩阵条件数良好,无需算子预处理(并且我们证明了关于 GMRES 收敛的相应结果)。这些结果的主要意义在于,最近已证明(参见 Chandler-Wilde 和 Spence,Numer. Math.,150(2):299-271,2022)存在二维和三维 Lipschitz 域以及三维星形 Lipschitz 多面体,使得 Laplace 方程的标准第二类积分方程公式(涉及双层势及其伴随)中的算子 $\textit{不能}$ 写成 $L^2(\Gamma)$ 空间中强制算子与紧算子之和。因此,存在二维和三维 Lipschitz 域以及三维星形 Lipschitz 多面体,使得 $L^2(\Gamma)$ 中的 Galerkin 方法应用于标准第二类公式时 $\textit{不}$ 收敛,但应用于新公式时 $\textit{确实}$ 收敛。

英文摘要:

We present new second-kind integral-equation formulations of the interior and exterior Dirichlet problems for Laplace's equation. The operators in these formulations are both continuous and coercive on general Lipschitz domains in $\mathbb{R}^d$, $d\geq 2$, in the space $L^2(Γ)$, where $Γ$ denotes the boundary of the domain. These properties of continuity and coercivity immediately imply that (i) the Galerkin method converges when applied to these formulations; and (ii) the Galerkin matrices are well-conditioned as the discretisation is refined, without the need for operator preconditioning (and we prove a corresponding result about the convergence of GMRES). The main significance of these results is that it was recently proved (see Chandler-Wilde and Spence, Numer. Math., 150(2):299-271, 2022) that there exist 2- and 3-d Lipschitz domains and 3-d starshaped Lipschitz polyhedra for which the operators in the standard second-kind integral-equation formulations for Laplace's equation (involving the double-layer potential and its adjoint) $\textit{cannot}$ be written as the sum of a coercive operator and a compact operator in the space $L^2(Γ)$. Therefore there exist 2- and 3-d Lipschitz domains and 3-d starshaped Lipschitz polyhedra for which Galerkin methods in $L^2(Γ)$ do $\textit{not}$ converge when applied to the standard second-kind formulations, but $\textit{do}$ converge for the new formulations.

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