双层楔形飞板爆炸反应装甲干扰聚能射流的数值模拟

刘迎彬 石军磊 胡晓艳 孙淼 张明 段晓畅

刘迎彬, 石军磊, 胡晓艳, 孙淼, 张明, 段晓畅. 双层楔形飞板爆炸反应装甲干扰聚能射流的数值模拟[J]. 高压物理学报, 2018, 32(4): 045105. doi: 10.11858/gywlxb.20170620
引用本文: 刘迎彬, 石军磊, 胡晓艳, 孙淼, 张明, 段晓畅. 双层楔形飞板爆炸反应装甲干扰聚能射流的数值模拟[J]. 高压物理学报, 2018, 32(4): 045105. doi: 10.11858/gywlxb.20170620
LIU Yingbin, SHI Junlei, HU Xiaoyan, SUN Miao, ZHANG Ming, DUAN Xiaochang. Numerical Simulation of Disturbance by Double-Layer Explosive Reactive Armor with Wedged Flying-Plate on Jet[J]. Chinese Journal of High Pressure Physics, 2018, 32(4): 045105. doi: 10.11858/gywlxb.20170620
Citation: LIU Yingbin, SHI Junlei, HU Xiaoyan, SUN Miao, ZHANG Ming, DUAN Xiaochang. Numerical Simulation of Disturbance by Double-Layer Explosive Reactive Armor with Wedged Flying-Plate on Jet[J]. Chinese Journal of High Pressure Physics, 2018, 32(4): 045105. doi: 10.11858/gywlxb.20170620

双层楔形飞板爆炸反应装甲干扰聚能射流的数值模拟

doi: 10.11858/gywlxb.20170620
基金项目: 

国家自然科学基金 11572292

详细信息
    作者简介:

    刘迎彬(1985-), 男, 博士, 讲师, 主要从事弹药毁伤防护与安全工程研究.E-mail:liuyb85@mail.ustc.edu.cn

    通讯作者:

    石军磊(1991-), 男, 硕士研究生, 主要从事聚能装药和装甲防护研究

  • 中图分类号: O389;TJ55

Numerical Simulation of Disturbance by Double-Layer Explosive Reactive Armor with Wedged Flying-Plate on Jet

  • 摘要: 为得到干扰聚能射流能力更好的爆炸反应装甲,在经典爆炸反应装甲的基础上,设计了一种双层楔形飞板爆炸反应装甲。利用ANSYS/LSDYNA-3D仿真软件对3种不同方案进行了模拟计算,分别对各方案中飞板飞行形态、逃逸射流特性、射流的动能变化以及聚能射流对靶板的侵彻深度进行了分析。结果表明:夹层炸药引爆后,楔形飞板在向外飞出的同时具有一定的旋转特征,合理的摆放结构能够增大飞板与射流的作用面积;聚能射流在穿过反应装甲后,动能急剧下降,穿深能力降低,方案二聚能射流侵彻深度最浅,方案三次之,方案一最深,表明方案二具有良好的防护效果。对楔形飞板的研究丰富了爆炸反应装甲的结构设计,为反应装甲的进一步研究提供了理论参考。

     

  • 图  模型示意(1.聚能战斗部;2.第1层ERA;3.第2层ERA;4.靶板)

    Figure  1.  Schematic of model (1.Shaped charge warhead; 2.First layer of ERA; 3.Second layer of ERA; 4.Target)

    图  有限元模型

    Figure  2.  Schematic of finite element models

    图  ERA尺寸(单位:cm)

    Figure  3.  ERA size (Unit:cm)

    图  ERA结构方案

    Figure  4.  ERA structure schemes

    图  40 μs时射流、ERA形态

    Figure  5.  Diagram of jet and ERA at 40 μs

    图  各方案不同时刻飞板的飞行形态

    Figure  6.  Pattern diagram of flying-plate for each scheme at different times

    图  各方案射流动能变化

    Figure  7.  Variation of kinetic energy of jetfor different schemes

    图  不同时刻各方案射流前导速度曲线

    Figure  8.  Variation of jet velocity fordifferent schemes at different times

    图  不同时刻各方案逃逸射流形态

    Figure  9.  State of escaped jet for different schemes at different times

    图  10  450 μs靶板侵彻深度

    Figure  10.  Depth of penetration of target at 450 μs

    表  1  B炸药材料模型及状态方程参数

    Table  1.   Parameters of material model and equation of state of explosive B

    ρ/(g·cm-3) pCJ/GPa D/(m·s-1) AJWL/GPa BJWL/GPa RJWL1 RJWL2 E0
    1.717 29.5 7 980 524.2 7.678 4.2 1.1 0.085
    下载: 导出CSV

    表  2  铜、钢材料模型及状态方程参数

    Table  2.   Parameters of material model and equation of state of copper and steel

    Material ρ/(g·cm-3) G/GPa AJ-C/GPa BJ-C/GPa S1 S2 C/(m·s-1) V0
    Copper 8.96 46 0.09 0.92 1.489 0 3 940 1
    Steel 7.785 77.5 0.175 0.376 1.49 0 4 570 1
    下载: 导出CSV

    表  3  夹层炸药的材料模型及状态方程参数

    Table  3.   Parameters of material model and equation of state of sandwich explosive

    ρ/(g·cm-3) G/GPa σY/GPa A/GPa B/GPa R1 R2 R3
    1.712 3.54 0.2 524.2 7.678 778.1 -5.031×10-2 2.223×10-5
    R5 R6 cP/(J·kg-1·K-1) cR/(J·kg-1·K-1) GROW2 AR2 ES1 ES2
    11.3 1.13 10-3 2.487×10-3 300 1 0.222 0.333
    下载: 导出CSV
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出版历程
  • 收稿日期:  2017-07-20
  • 修回日期:  2017-08-08

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