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

• Articles • 上一篇    下一篇

弹粘塑性材料中III型动态扩散裂纹尖端场的构造研究

贾斌1,王振清2,李永东3   

  1. 1.哈尔滨工业大学 复合材料与结构研究所,哈尔滨 150001;
    2.哈尔滨工程大学 建筑工程学院,哈尔滨 150001;
    3.装甲兵工程学院 机械工程系,北京 100072
  • 收稿日期:2007-09-29 修回日期:2008-05-27 出版日期:2008-07-03 发布日期:2008-01-01
  • 通讯作者: 贾斌

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

摘要: 采用弹粘塑性力学模型,对弹粘塑性材料中III型动态扩展裂纹尖端场进行了渐进分析,在线性硬化条件下,裂纹尖端的应力和应变场具有相同的幂奇异性,奇异性指数由材料的粘性
系数唯一确定。数值计算结果表明,运动参量裂纹扩展速度本身对裂纹尖场的分区构造影响较小。材料的硬化系数主导裂尖端的分区构造,但二次塑性区对裂尖场的影响较小。材料的粘性主导裂纹尖端应力和应变场的强度,同时对裂尖场的构造有一定的影响。当裂纹扩展速度为0时,动态解退化为相应的准静态解;当硬化系数为0时,线性硬化解还原为相应的理想塑性解。

关键词: 动态扩展裂纹, III型裂纹, 裂纹尖端场, 分区构造

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

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