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冲击荷载下运动裂纹与空孔相互作用的焦散线试验研究

骆浩浩 张渊通 左进京 李成孝 李炜煜

骆浩浩, 张渊通, 左进京, 李成孝, 李炜煜. 冲击荷载下运动裂纹与空孔相互作用的焦散线试验研究[J]. 矿业科学学报, 2022, 7(2): 210-216. doi: 10.19606/j.cnki.jmst.2022.02.008
引用本文: 骆浩浩, 张渊通, 左进京, 李成孝, 李炜煜. 冲击荷载下运动裂纹与空孔相互作用的焦散线试验研究[J]. 矿业科学学报, 2022, 7(2): 210-216. doi: 10.19606/j.cnki.jmst.2022.02.008
Luo Haohao, Zhang Yuantong, Zuo Jinjing, Li Chengxiao, Li Weiyu. Caustics experimental study on the interaction between moving cracks and voids under impact loading[J]. Journal of Mining Science and Technology, 2022, 7(2): 210-216. doi: 10.19606/j.cnki.jmst.2022.02.008
Citation: Luo Haohao, Zhang Yuantong, Zuo Jinjing, Li Chengxiao, Li Weiyu. Caustics experimental study on the interaction between moving cracks and voids under impact loading[J]. Journal of Mining Science and Technology, 2022, 7(2): 210-216. doi: 10.19606/j.cnki.jmst.2022.02.008

冲击荷载下运动裂纹与空孔相互作用的焦散线试验研究

doi: 10.19606/j.cnki.jmst.2022.02.008
基金项目: 

国家自然科学基金 51934001

详细信息
    作者简介:

    骆浩浩(1991—),男,河南正阳人,博士研究生,主要从事工程爆破和岩石破碎等方面的研究工作。Tel:13126973922,E-mail:1964423767@qq.com

  • 中图分类号: TU45

Caustics experimental study on the interaction between moving cracks and voids under impact loading

  • 摘要: 为了研究含有圆形缺陷的半圆盘试件在不同冲击速度下的断裂特征,采用霍普金森杆加载系统和动态焦散线试验系统,对半圆盘试件进行了试验研究。结果表明:裂纹起裂前,焦散斑半径出现跳跃情况,是入射杆的反复加载造成的;随着冲击速度的增加,裂纹穿过圆形缺陷的应力强度因子峰值有所增加,裂纹穿过圆形缺陷的扩展速度也增加明显;随着圆形缺陷半径的增大,裂纹在圆形缺陷处发生二次起裂时的应力强度因子变大。
  • 图  1  焦散成像示意图

    Figure  1.  Schematic diagram of caustics image

    图  2  SHPB和动态焦散线试验系统

    Figure  2.  SHPB and dynamic caustics test system diagram

    图  3  半圆盘弯曲试验示意图

    R—试件半径;d—厚度;a—裂纹长度; S—2个支撑点的距离;r—缺陷半径

    Figure  3.  Schematic diagram of semi-disc bending test

    图  4  运动裂纹与空孔相互作用动态焦散图

    Figure  4.  Dynamic caustics diagram of the interaction between moving cracks and voids

    图  5  缺陷半径1 mm时裂纹二次起裂的速度随时间变化曲线

    Figure  5.  When the defect radius is 1 mm, the speed of the second crack initiation varies with time

    图  6  缺陷半径1 mm时裂纹二次起裂的应力强度因子随时间变化关系曲线

    Figure  6.  When the defect radius is 1 mm, the intensity factor changes with time when the crack initiates a second time

    图  7  不同入射速度及不同孔径下裂纹二次起裂时的Kd

    Figure  7.  The Kd value of the second crack initiation under different incident speeds and different apertures

    表  1  有机玻璃力学参数

    Table  1.   Mechanical parameters of plexiglass

    参数 密度ρ/
    (kg·m-3)
    动态弹性
    模量Ed/GPa
    泊松比vd 纵波波速
    CP/(m·s-1)
    横波波速
    CS/(m·s-1)
    剪切模量
    G/GPa
    数值 1 180 6.1 0.31 2 320 1 260 1.28
    下载: 导出CSV

    表  2  不同入射速度及不同孔径下裂纹二次起裂时Kd

    Table  2.   Statistical table of Kd for the second crack initiation under different incident speeds and different apertures

    缺陷半径r/mm 二次起裂Kd/(MPa·m1/2)
    v1=2.7 m/s v2=2.3 m/s v3=2.2 m/s v4=2.0 m/s v5=1.5 m/s
    1.0 2.10 1.80 1.75 1.69 1.60
    1.5 2.30 2.20 1.90 1.80 1.70
    2.0 2.70 2.50 2.30 2.10 1.80
    2.5 3.60 3.20 2.90 2.60 2.30
    3.0 3.80 3.30 3.24 3.10 2.90
    下载: 导出CSV
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  • 收稿日期:  2021-01-13
  • 修回日期:  2021-01-21
  • 刊出日期:  2022-04-20

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