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Coupled fracture mode of a cracked disc under anti-plane loading

机译:抗平面载荷作用下裂纹盘的耦合断裂模式

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摘要

The existence of three-dimensional effects at cracks has been known for many years, but understanding has been limited, and for some situations still is. Understanding improved when the existence of corner point singularities and their implications became known. Increasingly powerful computers made it possible to investigate three-dimensional effects numerically in detail. Despite increased understanding, three-dimensional effects are sometimes ignored in situations where they may be important. The purpose of the present investigation is to study by means of accurate 3D finite element (FE) models a coupled fracture mode generated by anti-plane loading of a straight through-the-thickness crack in linear elastic discs. The results obtained from the highly accurate finite element analyses have improved understanding of the behaviour of through cracked discs under anti-plane loading. The influence of plate bending is increasingly important as disc thickness decreases. Bazant and Estenssoro's analysis works well for the symmetric mode (mode I), but it is incomplete for the asymmetric mode (a combination of modes II and III). It appears that a new field parameter, probably a singularity, is needed to describe the stresses at the disc surfaces. Discussion on whether K-III tends to zero or infinity as a corner point is approached is futile because K-III is meaningless at a corner point. Calculation of the strain energy density (SED) in a control volume at the crack tip shows that the position of the maximum SED is a function of disc thickness.
机译:裂缝处三维效应的存在已为人所知,但了解有限,在某些情况下仍然如此。当角点奇点的存在及其含义被人们所了解时,对理解的理解就会提高。功能越来越强大的计算机使对数字效果的三维细节研究成为可能。尽管有了更多的了解,但有时在某些情况下可能会忽略三维效果。本研究的目的是通过精确的3D有限元(FE)模型研究线性弹性圆盘中直通厚度的直裂纹的反平面载荷所产生的耦合断裂模式。从高度精确的有限元分析获得的结果使人们更好地了解了在抗平面载荷下直裂纹盘的行为。随着光盘厚度的减小,板弯曲的影响越来越重要。 Bazant和Estenssoro的分析对于对称模式(模式I)效果很好,但是对于非对称模式(模式II和III的组合)则不完整。似乎需要一个新的场参数(可能是奇点)来描述圆盘表面的应力。由于拐角处的K-III毫无意义,因此讨论接近拐角处K-III趋于零还是无穷大是徒劳的。在裂纹尖端的控制体积中的应变能密度(SED)的计算表明,最大SED的位置是圆盘厚度的函数。

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