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Analysis method of planar cracks of arbitrary shape in the isotropic plane of a three-dimensional transversely isotropic magnetoelectroelastic medium

机译:三维横向各向同性磁电弹性介质各向同性平面内任意形状的平面裂纹的分析方法

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The hyper-singular boundary integral equation method of crack analysis in three-dimensional transversely isotropic magnetoelectroelastic media is proposed. Based on the fundamental solutions or Green's functions of three-dimensional transversely isotropic magnetoelectroelastic media and the corresponding Somigliana identity, the boundary integral equations for a planar crack of arbitrary shape in the plane of isotropy are obtained in terms of the extended displacement discontinuities across crack faces. The extended displacement discontinuities include the displacement discontinuities, the electric potential discontinuity and the magnetic potential discontinuity, and correspondingly the extended tractions on crack face represent the conventional tractions, the electric displacement and the magnetic induction boundary values. The near crack tip fields and the intensity factors in terms of the extended displacement discontinuities are derived by boundary integral equation approach. A solution method is proposed by use of the analogy between the boundary integral equations of the magnetoelectroelastic media and the purely elastic materials. The influence of different electric and magnetic boundary conditions, i.e., electrically and magnetically impermeable and permeable conditions, electrically impermeable and magnetically permeable condition, and electrically permeable and magnetically impermeable condition, on the solutions is studied. The crack opening model is proposed to consider the real crack opening and the electric and magnetic fields in the crack cavity under combined mechanical-electric-magnetic loadings. An iteration approach is presented for the solution of the non-linear model. The exact solution is obtained for the case of uniformly applied loadings on the crack faces. Numerical results for a-square crack under different electric and magnetic boundary conditions are displayed to demonstrate the proposed method. (c) 2006 Elsevier Ltd. All rights reserved.
机译:提出了三维横观各向同性磁电弹性介质中裂纹分析的超奇异边界积分方程法。基于三维横观各向同性磁电弹性介质的基本解或格林函数以及相应的索米利亚纳身份,得出了各向同性平面内任意形状的平面裂纹的边界积分方程,该裂纹积分是通过裂纹面的扩展位移不连续性来实现的。 。扩展的位移不连续性包括位移不连续性,电势不连续性和磁势不连续性,并且相应地,裂纹面上的扩展牵引力代表常规牵引力,电位移和磁感应边界值。通过边界积分方程法导出了裂纹扩展场附近的尖端场和强度因子。利用磁电弹性介质与纯弹性材料的边界积分方程之间的类比,提出了一种求解方法。研究了不同的电和磁边界条件,即,电和磁不可渗透和可渗透的条件,电不可渗透和可磁渗透的条件,以及电可渗透和磁不可渗透的条件对解决方案的影响。提出了一种开裂模型,该模型考虑了真实的开裂以及在组合的机械-电磁负载下裂纹腔中的电场和磁场。针对非线性模型的求解,提出了一种迭代方法。对于在裂纹面上均匀施加载荷的情况,可以获得精确的解决方案。显示了在不同的电磁边界条件下a形裂纹的数值结果,以证明该方法。 (c)2006 Elsevier Ltd.保留所有权利。

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