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A unified definition for stress intensity factors of interface corners and cracks

机译:界面角和裂纹的应力强度因子的统一定义

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Based upon linear fracture mechanics, it is well known that the singular order of stresses near the crack tip in homogeneous materials is a constant value -1/2, which is nothing to do with the material properties. For the interface cracks between two dissimilar materials, the near tip stresses are oscillatory due to the order of singularity being -1/2 i epsilon and - 1/2. The oscillation index epsilon is a constant related to the elastic properties of both materials. While for the general interface corners, their singular orders depend on the corner angle as well as the elastic properties of the materials. Owing to the difference of the singular orders of homogeneous cracks, interface cracks and interface corners, their associated stress intensity factors are usually defined separately and even not compatibly. Since homogenous cracks and interface cracks are just special cases of interface corners, in order to build a direct connection among them a unified definition for their stress intensity factors is proposed in this paper. Based upon the analytical solutions obtained previously for the multibonded anisotropic wedges, the near tip solutions for the general interface corners have been divided into five different categories depending on whether the singular order is distinct or repeated, real or complex. To provide a stable and efficient computing approach for the general mixed-mode stress intensity factors, the path-independent H-integral based on reciprocal theorem of Betti and Rayleigh is established in this paper. The complementary solutions needed for calculation of H-integral are also provided in this paper. To illustrate our results, several different kinds of examples are shown such as cracks in homogenous isotropic or anisotropic materials, central or edge notches in isotropic materials, interface cracks and interface corners between two dissimilar materials. (c) 2007 Elsevier Ltd. All rights reserved.
机译:基于线性断裂力学,众所周知,均质材料中裂纹尖端附近的应力奇异阶为常数-1/2,这与材料特性无关。对于两种不同材料之间的界面裂纹,由于奇异度的顺序为-1/2 i和-1/2,因此近端应力是振荡的。振动指数ε是与两种材料的弹性有关的常数。对于一般的界面拐角,它们的奇异顺序取决于拐角以及材料的弹性。由于均质裂纹,界面裂纹和界面角的奇异顺序不同,它们的相关应力强度因子通常被单独定义,甚至不兼容。由于同质裂纹和界面裂纹只是界面角的特例,因此为了建立它们之间的直接连接,提出了应力强度因子的统一定义。基于先前针对多键各向异性楔块获得的解析解,根据奇异阶是不同的还是重复的,实数的还是复数的,用于一般界面角的近端解已分为五类。为了给一般的混合模应力强度因子提供稳定有效的计算方法,建立了基于贝蒂和瑞利互易定理的与路径无关的H积分。本文还提供了计算H积分所需的补充解。为了说明我们的结果,显示了几种不同类型的示例,例如均质各向同性或各向异性材料中的裂纹,各向同性材料中的中心或边缘缺口,两种不同材料之间的界面裂纹和界面角。 (c)2007 Elsevier Ltd.保留所有权利。

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