含氦泡辐照老化材料层裂损伤计算方法分析

张凤国 刘军 王言金 王裴 郑晖

张凤国, 刘军, 王言金, 王裴, 郑晖. 含氦泡辐照老化材料层裂损伤计算方法分析[J]. 爆炸与冲击, 2023, 43(10): 103105. doi: 10.11883/bzycj-2022-0486
引用本文: 张凤国, 刘军, 王言金, 王裴, 郑晖. 含氦泡辐照老化材料层裂损伤计算方法分析[J]. 爆炸与冲击, 2023, 43(10): 103105. doi: 10.11883/bzycj-2022-0486
ZHANG Fengguo, LIU Jun, WANG Yanjin, WANG Pei, ZHENG Hui. Simulation method of spall damage for self-radiation damage aging materials with helium bubbles[J]. Explosion And Shock Waves, 2023, 43(10): 103105. doi: 10.11883/bzycj-2022-0486
Citation: ZHANG Fengguo, LIU Jun, WANG Yanjin, WANG Pei, ZHENG Hui. Simulation method of spall damage for self-radiation damage aging materials with helium bubbles[J]. Explosion And Shock Waves, 2023, 43(10): 103105. doi: 10.11883/bzycj-2022-0486

含氦泡辐照老化材料层裂损伤计算方法分析

doi: 10.11883/bzycj-2022-0486
基金项目: 国家自然科学基金项目(12271054,12172063);科学挑战专题(TZ2018001)
详细信息
    作者简介:

    张凤国(1969- ),男,硕士,研究员,zhang_fengguo@iapcm.ac.cn

  • 中图分类号: O346.1

Simulation method of spall damage for self-radiation damage aging materials with helium bubbles

  • 摘要: 辐照条件下,一些材料内部产生大量的氦泡等微缺陷,氦泡的大小和数密度随着辐照年限的增长而增长。氦泡分布特征的变化不仅影响材料本身的物理、力学性质,而且直接影响材料层裂损伤演化后期材料破坏颗粒度的分布特征。延性材料的层裂损伤演化过程一般包括孔洞的成核、增长和汇合,但因已有孔洞对新成核孔洞存在抑制作用,当初始孔洞数密度达到一定临界值时,材料内部没有新的孔洞成核,因此,层裂损伤的计算可以不考虑新孔洞成核的影响。本文中基于损伤早期演化的特征,给出了这一临界值的计算方法,并进一步探讨了含氦泡辐照老化钚材料层裂损伤的计算方法。同时,在完善孔洞增长(void growth, VG)层裂损伤模型中参数的确定方法的基础上,借助含氦泡常规铝材料的层裂实验结果,对此问题进行了定性的分析:在氦泡尺寸变化不大的情况下,当氦泡浓度低于临界氦泡浓度时,需要考虑初始氦泡以及新增孔洞的综合影响;反之,可以采用简单的层裂损伤模型,不需要计算孔洞成核,但由于增长孔洞之间的相互影响,损伤模型的初始损伤参数需要重新确定。
  • 图  1  不同辐照老化年限钚材料中氦泡浓度和大小变化的实验统计结果[3]

    Figure  1.  Diameter and concentration of helium bubbles in self-irradiated plutonium during aging process[3]

    图  2  纯铝材料自由面速度曲线的实验[13]和数值模拟结果

    Figure  2.  Free surface velocities of experimental data[13] and simulation ones for pure aluminum

    图  3  含氦泡铝材料自由面速度曲线的实验[13]和数值模拟结果

    Figure  3.  Free surface velocities of experimental data[13] and simulation ones for pure aluminum with helium bubbles

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出版历程
  • 收稿日期:  2022-11-02
  • 修回日期:  2023-03-20
  • 刊出日期:  2023-10-27

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