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作为一个分岔问题的裂纹尖端过程区

Crack-tip process zone as a bifurcation problem.

作者信息

Boulbitch Alexei, Gufan Yury M, Korzhenevskii Alexander L

机构信息

IEE S.A. ZAE Weiergewan, 11, rue Edmond Reuter, L-5326 Contern, Luxembourg.

Institute for Physics, Stachki 194,344090 Rostov-on-Don, Russia.

出版信息

Phys Rev E. 2017 Jul;96(1-1):013005. doi: 10.1103/PhysRevE.96.013005. Epub 2017 Jul 24.

Abstract

Stress concentration at a crack tip generates a solid structural transformation in its vicinity, the process zone. We argue that its formation represents a local phase transition described by a multicomponent order parameter. We derive a system of equations describing the dynamics of the order parameter driven by an inhomogeneous, time-dependent stress field in the solid and show that it exhibits a bifurcation. The latter corresponds to the emergence of a process zone characterized by the distribution of the order parameter localized in the vicinity of the crack tip. The emergence temperature T_{} considerably differs from the temperature of the bulk phase transformation T_{c}. We demonstrate that T_{} exhibits a universal behavior T_{*}-T_{c}∼K_{I}^{4/3}, in terms of the stress intensity factor K_{I}, and that the zone universally vanishes upon achieving a critical velocity. These facts together give rise to a universal dynamic phase diagram.

摘要

裂纹尖端的应力集中会在其附近即过程区产生一种固体结构转变。我们认为其形成代表了一种由多分量序参量描述的局部相变。我们推导了一组方程,该方程描述了由固体中不均匀的、随时间变化的应力场驱动的序参量的动力学,并表明它呈现出一种分岔现象。后者对应于一个过程区的出现,该过程区的特征是序参量分布集中在裂纹尖端附近。出现温度(T_{})与体相转变温度(T_{c})有很大差异。我们证明,就应力强度因子(K_{I})而言,(T_{})呈现出(T_{*}-T_{c}∼K_{I}^{4/3})的普适行为,并且该区域在达到临界速度时会普遍消失。这些事实共同产生了一个普适的动态相图。

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