Applied Mathematics and Mechanics (English Edition) ›› 2008, Vol. 29 ›› Issue (7): 919-925 .doi: https://doi.org/10.1007/s10483-008-0710-x

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Field structure at mode III dynamically propagating crack tip in elastic-viscoplastic materials

JIA Bin1, WANG Zhen-qing2 , LI Yong-dong3   

  1. 1. Center for Composite Materials, Harbin Institute of Technology,Harbin 150001, P. R. China;
    2. Architectural Engineering College, Harbin Engineering University,Harbin 150001, P. R. China;
    3. Mechanical Engineering Department, Armored Forces Engineering Institute,Beijing 100072, P. R. China
  • Received:2007-09-29 Revised:2008-05-27 Online:2008-07-03 Published:2008-01-01
  • Contact: JIA Bin

Abstract: An elastic-viscoplastic mechanics model is used to investigate asymptotically the mode III dynamically propagating crack tip field in elastic-viscoplastic materials. The stress and strain fields at the crack tip possess the same power-law singularity under a linear-hardening condition. The singularity
exponent is uniquely determined by the viscosity coefficient of the material. Numerical results indicate that the motion parameter of the crack propagating speed has little effect on the zone structure at the crack tip. The hardening
coefficient dominates the structure of the crack-tip field. However, the secondary plastic zone has little influence on the field. The viscosity of the material dominates the strength of stress and strain fields at the crack tip while it does have certain influence on the crack-tip field structure. The dynamic crack-tip field degenerates into the relevant quasi-static solution when the crack moving speed is zero. The corresponding perfectly-plastic
solution is recovered from the linear-hardening solution when the hardening coefficient becomes zero.

Key words: elastic-viscoplastic materials, dynamically propagating crack, mode III crack, crack tip field, zone structure

2010 MSC Number: 

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