基于细观建模的电子束预控弹体破裂机理数值研究

邱浩 蒋建伟 门建兵 王树有 李梅

邱浩, 蒋建伟, 门建兵, 王树有, 李梅. 基于细观建模的电子束预控弹体破裂机理数值研究[J]. 爆炸与冲击, 2021, 41(7): 074201. doi: 10.11883/bzycj-2020-0220
引用本文: 邱浩, 蒋建伟, 门建兵, 王树有, 李梅. 基于细观建模的电子束预控弹体破裂机理数值研究[J]. 爆炸与冲击, 2021, 41(7): 074201. doi: 10.11883/bzycj-2020-0220
QIU Hao, JIANG Jianwei, MEN Jianbing, WANG Shuyou, LI Mei. Numerical study on the fracture mechanism of electron beam controlled projectile based on micro modeling[J]. Explosion And Shock Waves, 2021, 41(7): 074201. doi: 10.11883/bzycj-2020-0220
Citation: QIU Hao, JIANG Jianwei, MEN Jianbing, WANG Shuyou, LI Mei. Numerical study on the fracture mechanism of electron beam controlled projectile based on micro modeling[J]. Explosion And Shock Waves, 2021, 41(7): 074201. doi: 10.11883/bzycj-2020-0220

基于细观建模的电子束预控弹体破裂机理数值研究

doi: 10.11883/bzycj-2020-0220
基金项目: 国家自然科学基金(11872123)
详细信息
    作者简介:

    邱 浩(1990- ),男,博士研究生,qiuhaomail@foxmail.com

    通讯作者:

    蒋建伟(1963- ),男,博士,教授,bitjjw@bit.edu.cn

  • 中图分类号: O389; TJ413

Numerical study on the fracture mechanism of electron beam controlled projectile based on micro modeling

  • 摘要: 为研究电子束预控弹体的破裂机理。提出了基于电子束预控弹体细观几何特性的参数化建模方法,建立了含基体、熔融区、过渡区和空腔区弹体的三维有限元模型,采用LS-DYNA软件对典型弹体的爆炸驱动和破裂过程进行了数值模拟分析。结果表明:电子束预控弹体破裂过程可分为:弹体膨胀后的空腔区在环向拉应力作用下产生拉伸断裂、过渡区产生裂纹扩展和拉伸断裂以及空腔区底部基体在两侧拉应力和底部压应力作用下产生与弹体内壁法线呈45°的剪切破坏3个阶段。数值模拟结果与回收的破片截面形状和破坏模式吻合较好。研究结果对电子束预控弹体破片成型控制具有参考价值。
  • 图  1  电子束预控区域

    Figure  1.  Electron beam controlled zone

    图  2  电子束预控区域示意

    Figure  2.  Schematic of electron beam controlled zone

    图  3  硬度值沿纵横向距离的关系

    Figure  3.  Relationship of hardness value along the vertical and horizontal distance

    图  4  典型电子束预控弹体的几何特征参数

    Figure  4.  Geometric characteristic parameters of typical electron beam controlled projectile

    图  5  槽线相交菱形的边长

    Figure  5.  Side length of rhombus with groove lines intersecting

    图  6  单个槽网格数量示意图

    Figure  6.  Schematic diagram of the number of grids in a single groove

    图  7  周向移动节点

    Figure  7.  Circumferential mobile node

    图  8  端部节点的生成

    Figure  8.  Generation of end nodes

    图  9  电子束预控弹体离散化模型

    Figure  9.  Finite element model of electron beam controlled projectile

    图  10  典型电子束预控弹体和选取的局部区域

    Figure  10.  The typical electron beam controlled projectile and the selected local area

    图  11  电子束预控弹体不同计算时刻应力云图

    Figure  11.  Contours of Pressure of electron beam controlled projectile with different time

    图  12  弹体内的应力分量

    Figure  12.  The stress components in the projectile

    图  13  空腔区受力分析

    Figure  13.  Stress analysis of hollow zone

    图  14  12 μs时刻预控破片截面图像与回收破片截面

    Figure  14.  Section image of controlled fragments at 12 μs and section of recycled fragment

    表  1  测量的硬度值

    Table  1.   Measured hardness value

    区域维氏硬度
    横向410410425415413406
    369324330369376
    纵向391391386392403
    基体366361372
    下载: 导出CSV

    表  2  35CrMnSi Johnson-Cook本构模型参数[14]

    Table  2.   Parameters of Johnson-Cook constitutive equation for 35CrMnSi[14]

    ρ0/(g·cm−3G/GPaA/MPaB/MPanCmTm/K
    7.8377144015010.44030.0390.4041793
    下载: 导出CSV

    表  3  COMP B炸药的JWL状态方程参数[15]

    Table  3.   Parameters of JWL equation of state for COMP B explosive[15]

    ρ0/(g·cm−3A/GPaB/GPaR1R2ωD/(m·s−1pCJ/GPaE/(GJ·m−3
    1.7125.24230.076784.21.10.3479800.2950.085
    下载: 导出CSV
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出版历程
  • 收稿日期:  2020-07-01
  • 修回日期:  2020-09-25
  • 网络出版日期:  2021-07-05
  • 刊出日期:  2021-07-05

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