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The Singular Function Boundary Integral Method for the 2-D and 3-D Laplace Equation Problems in Mechanics, with a Boundary Singularity

机译:具有边界奇异性的二维2-D和3-D拉普拉斯方程问题的奇异函数边界积分方法

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In this study the Singular Function Boundary Integral Method (SFBIM) is implemented in the case of a planar elliptic boundary value problem in Mechanics, with a point boundary singularity. The method is also extended in the case of a typical problem of Solid Mechanics, concerning the Laplace equation problem in three dimensions, defined in a domain with a straight edge singularity on the surface boundary. In both the 2-D and 3-D cases, the general solution of the Laplace equation is approximated by the leading terms (which contain the singular functions) of the local asymptotic solution expansion. The singular functions are used to weight the governing equation in the Galerkin sense. For the 2-D Laplacian model problem of this study, which is defined over a domain with a re-entrant corner, the resulting discretized equations are reduced to boundary integrals by means of Green's second identity. For the 3-D model problem of this work, the volume integrals of the discretized equations are reduced to surface integrals by implementing Gauss' divergence theorem. The Dirichlet boundary conditions are then weakly enforced by means of Lagrange multipliers. The values of the latter are calculated together with the singular coefficients, in the 2-D case or the Edge Flux Intensity Functions (EFIFs), in the 3-D model problem, which appear in the local solution expansion. For the planar problem, the numerical results are favorably compared with the analytic solution. Especially for the extension of the method in three dimensions, the preliminary numerical results compare favorably with available postprocessed finite element results.
机译:在这项研究中,在具有点边界奇异性的力学中,采用平面椭圆边界值问题的情况下,采用奇异函数边界积分方法(SFBIM)。在固体力学的典型问题的情况下,该方法也得到了扩展,涉及三维Laplace方程问题,该问题在表面边界上具有直边奇异性的区域中定义。在2-D和3-D情况下,拉普拉斯方程的一般解都通过局部渐近解展开的前导项(包含奇异函数)来近似。奇异函数用于加权Galerkin意义上的控制方程。对于本研究的二维Laplacian模型问题(定义在具有凹角的区域上),所得离散化方程通过格林的第二恒等式简化为边界积分。对于这项工作的3D模型问题,通过实施高斯散度定理,离散方程的体积积分被简化为表面积分。然后通过拉格朗日乘数弱地执行Dirichlet边界条件。后者的值与2D情况下的奇异系数或在3D模型问题中出现在局部解扩展中的边缘通量强度函数(EFIF)一起计算。对于平面问题,将数值结果与解析解进行了比较。特别是对于该方法在三个维度上的扩展,初步数值结果与可用的后处理有限元结果相比具有优势。

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