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Unique real-variable expressions of displacement and traction fundamental solutions covering all transversely isotropic elastic materials for 3D BEM

机译:位移和牵引力基本解的唯一实变量表达式,涵盖了3D BEM的所有横向各向同性弹性材料

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A general, efficient and robust boundary element method (BEM) formulation for the numerical solution of three-dimensional linear elastic problems in transversely isotropic solids is developed in the present work. The BEM formulation is based on the closed-form real-variable expressions of the fundamental solution in displacements U-ik and in tractions T-ik, originated by a unit point force, valid for any combination of material properties and for any orientation of the radius vector between the source and field points. A compact expression of this kind for Uik was introduced by Ting and Lee (Q. J. Mech. Appl. Math. 1997; 50:407-426) in terms of the Stroh eigenvalues on the oblique plane normal to the radius vector. Working from this expression of U-ik, and after a revision of their final formula, a new approach (based on the application of the rotational symmetry of the material) for deducing the derivative kernel U-ik,U-j and the corresponding stress kernel Sigma(ijk) and traction kernel T-ik has been developed in the present work. These expressions of U-ik, U-ik,U-j, Sigma(ijk) and T-ik do not suffer from the difficulties of some previous expressions, obtained by other authors in different ways, with complex-valued functions appearing for some combinations of material parameters and/or with division by zero for the radius vector at the rotational-symmetry axis. The expressions of U-ik, U-ik,U-j, Sigma(ijk) and T-ik have been presented in a form suitable for an efficient computational implementation. The correctness of these expressions and of their implementation in a three-dimensional collocational BEM code has been tested numerically by solving problems with known analytical solutions for different classes of transversely isotropic materials. Copyright (c) 2007 John Wiley & Sons, Ltd.
机译:在目前的工作中,开发了一种通用,有效和鲁棒的边界元方法(BEM)公式,用于求解横观各向同性固体中的三维线性弹性问题。 BEM公式基于位移U-ik和牵引力T-ik中基本解的闭式实变量表达式,该表达式由单位点力产生,对材料特性的任何组合和材料的任何方向均有效。源点和场点之间的半径向量。 Ting和Lee(Q. J. Mech。Appl。Math。1997; 50:407-426)根据垂直于半径矢量的斜面上的Stroh特征值,为Uik引入了这种紧凑表达式。从U-ik的这种表达式出发,并在修改其最终公式后,得出了一种新方法(基于材料旋转对称的应用),以推导导数核U-ik,Uj和相应的应力核Sigma (ijk)和牵引内核T-ik已在当前工作中开发。 U-ik,U-ik,Uj,Sigma(ijk)和T-ik的这些表达式没有遭受其他作者以不同方式获得的某些先前表达式的困难,对于某些组合,出现了复数值函数材料参数和/或旋转对称轴上的半径矢量除以零。 U-ik,U-ik,U-j,Sigma(ijk)和T-ik的表达形式适合于有效的计算实现。这些表达式的正确性及其在三维搭配BEM代码中的实现已通过解决已知的解析方法对不同种类的横向各向同性材料的问题进行了数值测试。版权所有(c)2007 John Wiley&Sons,Ltd.

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