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Generalized finite element method for second-order elliptic operators with Dirichlet boundary conditions

机译:Dirichlet边界条件的二阶椭圆算子的广义有限元方法

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摘要

We introduce a method for approximating essential boundary conditions-conditions of Dirichlet type-within the generalized finite element method (GFEM) framework. Our results apply to general elliptic boundary value problems of the form -Sigma(n)(i,j=1) (a(ij) u(xi))x(j) + Sigma(n)(i=1) b(i)u(xi) + cu = f in Omega, u=0 on partial derivative Omega, where Omega is a smooth bounded domain. As test-trial spaces, we consider sequences of GFEM spaces, {S-mu}(mu >= 1), which are nonconforming (that is S-mu not subset of H-0(1)(Omega)). We assume that parallel to nu parallel to(L2(partial derivative Omega)) <= Ch(mu)(m)parallel to nu parallel to(H1(Omega)), for all v is an element of S-mu, and there exists u(1) is an element of S-mu, such that parallel to u-u(1)parallel to(H1(Omega)) <= Ch(mu)(j)parallel to u parallel to(Hj+1(Omega)), 0 <= j <= m, where u is an element of Hm+1(Omega) is the exact solution, m is the expected order of approximation, and hp is the typical size of the elements defining S, Under these conditions, we prove quasi-optimal rates of convergence for the GFEM approximating sequence up E S, of u. Next, we extend our analysis to the inhomogeneous boundary value problem -Sigma(n)(i,j=1)(a(ij)u(xi))(xj) + Sigma(n)(i=1) b(i)u(xi) + cu = f in Omega, u =g on partial derivative Omega. Finally, we outline the construction of a sequence of GFEM spaces S-mu subset of (S) over tilde (mu), mu = 1, 2,..., that satisfies out assumptions. (C) 2007 Published by Elsevier B.V.
机译:我们介绍了一种在广义有限元方法(GFEM)框架内逼近Dirichlet类型基本条件的方法。我们的结果适用于形式为-Sigma(n)(i,j = 1)(a(ij)u(xi))x(j)+ Sigma(n)(i = 1)b(在Omega中,i)u(xi)+ cu = f,在偏导数Omega中,u = 0,其中Omega是光滑有界域。作为测试空间,我们考虑了不符合标准的GFEM空间序列{S-mu}(mu> = 1)(即S-mu不是H-0(1)Omega的子集)。我们假设平行于nu平行于(L2(偏导数Omega))<= Ch(mu)(m)平行于nu平行于(H1Omega)),因为所有v都是S-mu的元素,并且存在u(1)是S-mu的元素,因此平行于uu(1)平行于(H1(Omega))<= Ch(mu)(j)平行于u平行于(Hj + 1(Omega) ),0 <= j <= m,其中u是Hm + 1(Omega)的元素是精确解,m是期望的近似阶数,hp是定义S的元素的典型大小,我们证明了u的GFEM近似序列的准最优收敛速度。接下来,我们将分析扩展到不均匀边值问题-Sigma(n)(i,j = 1)(a(ij)u(xi))(xj)+ Sigma(n)(i = 1)b(i )u(xi)+ cu =Ω(在Omega中),u = g(在偏导数Omega上)。最后,我们概述了满足假设的GFEM空间序列(S)的S-mu子集,代字号(mu),mu = 1,2,...。 (C)2007由Elsevier B.V.发布

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