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Effect of the discreteness of the atomic structure on cleavage crack extension in brittle crystalline materials

机译:原子结构的离散性对脆性晶体材料中裂解裂纹扩展的影响

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Elliott's model of a straight‐fronted cleavage crack is used to conduct an analytical Peierls‐Nabarro‐type calculation appropriate for a two‐dimensional lattice where the atomic spacings are respectively a and b normal and parallel to the cleavage crack. The analysis enables the effect of the discreteness of the atomic structure on brittle cleavage crack extension to be assessed and circumvents some of the limitations in a previous analysis due to Thomson, Hsieh, and Rana. The general conclusion emerging from the present work is that the magnitude of the discreteness effect, reflected in the ratio between the crack extension stress and that predicted by the continuum‐based Griffith relation, is greater the smaller the crack front width which thereby substantiates Thomson, Hsieh, and Rana's inferences. Proceeding from this conclusion, the wider problem of relating the magnitude of the discreteness effect, crack front width, and the type of atomic bonding is discussed from an essentially physical viewpoint. As a result of such considerations it is suggested that, in general, the discreteness effect will be small and the crack front will be wide with a material that is more resistant to elastic shear than tension, as in a covalently bonded solid where the bonding is directional. Since dislocation mobility is difficult in such a material, it would therefore seem that existing arguments regarding brittle cleavage crack extension should not be significantly affected by the introduction of discreteness considerations and that very special circumstances are likely to be required to give a large discreteness effect, as would be reflected in a brittle crack extension stress markedly in excess of that predicted by the Griffith relation.
机译:使用Elliott的直前裂隙裂纹模型进行解析Peierls-Nabarro型计算,该计算适用于原子间距分别为a和b且平行于裂隙裂纹的二维晶格。通过该分析,可以评估原子结构的离散性对脆性裂解裂纹扩展的影响,并且可以避免由于Thomson,Hsieh和Rana而导致的先前分析中的某些限制。从目前的工作中得出的一般结论是,在裂纹扩展应力与基于连续谱的格里菲斯(Griffith)关系所预测的比例之间反映出的离散效应的幅度越大,裂纹前缘宽度越小,从而证实了汤姆森,谢和拉娜的推论。从这个结论出发,从本质上的物理角度讨论了有关离散效应的大小,裂纹前沿宽度和原子键类型的更广泛的问题。考虑到这些因素,通常认为,与共价键结合的固体相比,使用弹性比拉伸力更强的材料时,离散效应将很小,并且裂纹前沿将变宽。定向的。由于在这种材料中难于进行位错迁移,因此,关于脆性解理裂纹扩展的现有论据似乎不会受到引入离散性因素的影响,并且可能需要非常特殊的情况才能产生较大的离散性效应,正如脆性裂纹扩展应力明显超过格里菲斯关系所预测的那样。

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    《Journal of Applied Physics》 |1974年第5期|P.2039-2045|共7页
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  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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