...
首页> 外文期刊>International Journal of Solids and Structures >M-integral analysis for two-dimensional solids with strongly interacting microcracks. Part I: in an infinite brittle solid
【24h】

M-integral analysis for two-dimensional solids with strongly interacting microcracks. Part I: in an infinite brittle solid

机译:具有强烈相互作用的微裂纹的二维固体的M积分分析。第一部分:在无限脆性固体中

获取原文
获取原文并翻译 | 示例

摘要

This paper addresses an alternative description for brittle solids with strongly interacting microcracks. The basic idea starts from the M-integral analysis customarily used in single crack problems. As an initial attempt, the discussion is limited to the infinite two-dimensional cases and the microcracks are assumed to be stationary. It is proved from the global-local coordinate translations that the M integral is divided into two distinct parts. First of them is induced from the well-known relation between the integral and the stress intensity factors (SIFs) at all the crack tips (Freund, 1978). The second is contributed from the two components of the J(k) vector (Knowles and Sternberg, 1972, Budiansky and Rice, 1973) and the coordinates of each microcrack center. The later is concerned not only with the crack tip SIFs, but also with the contribution arising from the traction-free surfaces of each crack (Herrmann and Herrmann, 1981). A detailed proof for the vanishing nature of the J(k) vector along a closed contour surrounding all the microcracks is presented, from which the confusion about the dependence of the M integral on the origin selection of global coordinates is clarified. Two numerical examples are shown in tables and figures to confirm the derived conclusions. It is shown that the M integral is equivalent to the decrease of the total potential energy of the microcracking solids although the strongly interacting situations are taken into account. Therefore, a simple relation between the M integral and the L integral is established under the assumption mentioned above. It is concluded that the M-integral analysis, from the physical point of view, does play important role and provide an effective measure in evaluating the damage level of brittle solids with strongly interacting and randomly distributed microcracks. Although only the stationary microcracks are considered in the present investigation, the derived conclusions could actually be extended to treat much more useful problems, in which the multi-cracks may become critical and may grow during loading histories. (C) 2001 Elsevier Science Ltd. All rights reserved. [References: 34]
机译:本文讨论了具有强烈相互作用的微裂纹的脆性固体的替代描述。基本思想始于通常在单裂纹问题中使用的M积分分析。作为最初的尝试,讨论仅限于无限的二维情况,并且假定微裂纹是固定的。从全局-局部坐标转换可以证明,M积分分为两个不同的部分。首先,它们是由所有裂纹尖端处的积分和应力强度因子(SIF)之间的众所周知的关系引起的(Freund,1978年)。第二个是由J(k)向量的两个分量(Knowles和Sternberg,1972; Budiansky和Rice,1973)和每个微裂纹中心的坐标贡献的。后者不仅与裂纹尖端的SIF有关,而且与每个裂纹的无牵引表面产生的影响有关(Herrmann和Herrmann,1981)。给出了关于J(k)向量沿着围绕所有微裂纹的闭合轮廓消失的详细证明,由此澄清了关于M积分对全局坐标原点选择的依赖性的混淆。在表和图中显示了两个数值示例,以确认得出的结论。结果表明,尽管考虑了强烈相互作用的情况,但M积分等于微裂纹固体总势能的降低。因此,在上述假设下,建立M积分和L积分之间的简单关系。结论是,从物理角度来看,M积分分析的确发挥了重要作用,并为评估脆性固体的强相互作用和随机分布的微裂纹的破坏程度提供了有效的措施。尽管在本研究中仅考虑了固定的微裂纹,但实际上可以将得出的结论扩展到治疗更有用的问题,在这些问题中,多裂纹可能变得很关键,并且在加载历史中可能会增长。 (C)2001 Elsevier ScienceLtd。保留所有权利。 [参考:34]

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号