Numerical Evaluation of Stress Intensity Factor for Inclined-Edge Crack Geometry using Singularity Elements

N. Tatke, N. Kotkunde
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Abstract

Edge cracks are more dangerous than interior cracks. Free edge close to the crack influences the stress field near the crack tip (since the free edge is traction free).In case of edge crack, the free edge is not only close to the crack, but it intersects the crack. Evaluation of Stress Intensity factor for oblique edge crack geometry is done using commercial FEM software ANSYS and compared with analytical results. The conventional elements always underestimate the sharply rising stress-displacement gradients near the crack tip. Therefore, in order to produce this singularity in stresses and strains Barsoum elements were employed which involves shifting the mid-side nodes to the quarter point locations. It observed that stress intensity factor found by FEM method has good agreement with analytical results.. The singular order of stresses near the interface is a good way of understanding of failure initiation; however, in engineering applications usually the knowledge of singular orders is not enough for the prediction of failure initiation. As an example in the case of homogeneous cracks, the singular order is -1/2 which remains constant irrespective of the surrounding environment and outside loading of the crack. These influential factors are reflected through the associated stress intensity factor of the cracks. Hwu and Kuo [1] have demonstrated several different kinds of examples 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. It is also shown that KI Evaluation Using Displacement etrapolation technique under adaptive dense mesh with Parallel Finite Element gives fairly accurate results [2]. Based upon the analytical solutions obtained previously for the multi-bonded anisotropic wedges and the well-known path-independent H-integral, Hwo and Kuo [3] provided a unified definition and a stable computing approach for the stress intensity factors of interface corners. The stress intensity factor calculations are usually limited to Linear Elastic Fracture Mechanics (LEFM). For a linear elastic material the stress and strain fields ahead of the crack tip are expressed as [4]. The singular order of stresses near the interface is a good way of understanding of failure initiation; however, in engineering applications usually the knowledge of singular orders is not enough for the prediction of failure initiation. As an example in the case of homogeneous cracks, the singular order is -1/2 which remains constant irrespective of the surrounding environment and outside loading of the crack. These influential factors are reflected through the associated stress intensity factor of the cracks. Hwu and Kuo [1] have demonstrated several different kinds of examples 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. It is also shown that KI Evaluation Using Displacement etrapolation technique under adaptive dense mesh with Parallel Finite Element gives fairly accurate results [2]. Based upon the analytical solutions obtained previously for the multi-bonded anisotropic wedges and the wellknown path-independent H-integral, Hwo and Kuo [3] provided a unified definition and a stable computing approach for the stress intensity factors of interface corners. The stress intensity factor calculations are usually limited to Linear Elastic Fracture Mechanics (LEFM). For a linear elastic material the stress and strain fields ahead of the crack tip are expressed as [4].
基于奇异元的斜边裂纹几何应力强度因子数值计算
边缘裂缝比内部裂缝更危险。靠近裂纹的自由边影响裂纹尖端附近的应力场(因为自由边不受牵引)。在边缘裂纹情况下,自由边不仅靠近裂纹,而且与裂纹相交。利用商业有限元软件ANSYS对斜边裂纹几何形状的应力强度因子进行了评估,并对分析结果进行了比较。传统的单元总是低估裂纹尖端附近急剧上升的应力-位移梯度。因此,为了产生应力和应变的奇异性,采用了Barsoum单元,其中包括将中间节点移动到四分之一点位置。结果表明,有限元法得到的应力强度因子与分析结果吻合较好。界面附近应力的奇异顺序是理解破坏起裂的好方法;然而,在工程应用中,单阶的知识通常不足以预测故障的发生。以均质裂纹为例,奇异阶数为-1/2,无论裂纹周围环境和外部荷载如何,奇异阶数都保持不变。这些影响因素通过裂纹的相关应力强度因子反映出来。Hwu和Kuo[1]已经展示了几种不同类型的例子,如均匀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。采用平行有限元自适应密集网格下的位移推算技术进行KI评价,得到了较为准确的结果[2]。hho和Kuo[3]基于多键各向异性楔块的解析解和众所周知的与路径无关的h积分,为界面角的应力强度因子提供了统一的定义和稳定的计算方法。应力强度因子的计算通常局限于线弹性断裂力学(LEFM)。对于线弹性材料,裂纹尖端前的应力和应变场表示为[4]。界面附近应力的奇异顺序是理解破坏起裂的好方法;然而,在工程应用中,单阶的知识通常不足以预测故障的发生。以均质裂纹为例,奇异阶数为-1/2,无论裂纹周围环境和外部荷载如何,奇异阶数都保持不变。这些影响因素通过裂纹的相关应力强度因子反映出来。Hwu和Kuo[1]已经展示了几种不同类型的例子,如均匀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。采用平行有限元自适应密集网格下的位移推算技术进行KI评价,得到了较为准确的结果[2]。hho和Kuo[3]基于多键各向异性楔块的解析解和众所周知的与路径无关的h积分,为界面角的应力强度因子提供了统一的定义和稳定的计算方法。应力强度因子的计算通常局限于线弹性断裂力学(LEFM)。对于线弹性材料,裂纹尖端前的应力和应变场表示为[4]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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