延时起爆对串联EFP成型及其侵彻效应的影响

徐浩铭 顾文彬 曾政 王振雄 赵长啸

徐浩铭, 顾文彬, 曾政, 王振雄, 赵长啸. 延时起爆对串联EFP成型及其侵彻效应的影响[J]. 高压物理学报, 2014, 28(1): 79-85. doi: 10.11858/gywlxb.2014.01.013
引用本文: 徐浩铭, 顾文彬, 曾政, 王振雄, 赵长啸. 延时起爆对串联EFP成型及其侵彻效应的影响[J]. 高压物理学报, 2014, 28(1): 79-85. doi: 10.11858/gywlxb.2014.01.013
XU Hao-Ming, GU Wen-Bin, ZENG Zheng, WANG Zhen-Xiong, ZHAO Chang-Xiao. Effect of Delay Time on Formation and Penetration of Tandem EFP[J]. Chinese Journal of High Pressure Physics, 2014, 28(1): 79-85. doi: 10.11858/gywlxb.2014.01.013
Citation: XU Hao-Ming, GU Wen-Bin, ZENG Zheng, WANG Zhen-Xiong, ZHAO Chang-Xiao. Effect of Delay Time on Formation and Penetration of Tandem EFP[J]. Chinese Journal of High Pressure Physics, 2014, 28(1): 79-85. doi: 10.11858/gywlxb.2014.01.013

延时起爆对串联EFP成型及其侵彻效应的影响

doi: 10.11858/gywlxb.2014.01.013
基金项目: 国家科技支撑计划项目(2012BAK05B01)
详细信息
    作者简介:

    徐浩铭(1985-), 男, 博士研究生, 主要从事弹药工程研究.E-mail:xuhaoming2012@sina.com

  • 中图分类号: O385;TJ410.3

Effect of Delay Time on Formation and Penetration of Tandem EFP

  • 摘要: 为了解决在大块度障碍物上快速开孔且孔深和孔径符合要求的难题,提出了一种前、后两级均为爆炸成型弹丸(EFP)装药的新型串联聚能装药结构。利用LS-DYNA3D有限元软件,对串联EFP装药的成型过程进行了数值仿真,分析了两级装药延时起爆对后级EFP成型的影响,并在此基础上开展了串联EFP装药侵彻45钢靶实验。结果表明:该串联EFP装药结构可充分发挥前、后两级EFP的侵彻能力,提高了侵彻效果。

     

  • 图  微秒起爆控制系统

    Figure  1.  Microsecond detonation control system

    图  串联EFP装药的整体模型

    Figure  2.  The whole model of tandem EFP charge

    图  不同炸高条件下EFP侵彻钢靶的数值模拟与实验结果对比

    Figure  3.  Comparison of simulated and experimental results of steel target penetrated by EFP at various height of burst

    图  4(a)  后级EFP的最大速度与装药间距的关系

    Figure  4(a).  Relationship between maximum velocity of postpositive EFP and interval distance

    图  4(b)  后级EFP的长径比与装药间距的关系

    Figure  4(b).  Relationship between the length to diameter ratio and interval distance

    图  串联EFP装药侵彻钢靶仿真(b=200 mm)

    Figure  5.  Numerical simulation of tandem EFP charge penetrating the steel target (b=200 mm)

    图  实验设置

    Figure  6.  Experimental set-up

    图  串联EFP装药侵彻钢靶实验结果

    Figure  7.  Experimental results of tandem EFP charge penetrating the steel target

    图  数值模拟与实验结果的对比

    Figure  8.  Comparison of numerical simulation and experimental results

    表  1  炸药的计算参数

    Table  1.   Computation parameters of explosive

    ρ/(g/cm3) v/(km/s) pCJ/(GPa) E0/(GPa) A/(GPa) B/(GPa) R1 R2 ω
    1.70 8.4 30 10.0 56.4 6.801 4.1 1.3 0.36
    下载: 导出CSV

    表  2  紫铜药型罩的计算参数

    Table  2.   Computation parameters of copper liner

    ρ/(g/cm3) C/(km/s) S1 S2 S3 γ0 a E0/(GPa)
    8.96 4.75 3.8 2.74 0.125 1.346 0.34 0.0
    下载: 导出CSV

    表  3  不同炸高条件下侵彻深度和穿孔直径的数值模拟结果和实验结果

    Table  3.   Simulated and experimental results of penetration depth and expanded diameter at various height of burst

    H/(mm) P/R d/R
    Sim. Exp. Sim. Exp.
    150 0.73 0.74 0.557 0.563
    180 0.80 0.78 0.525 0.530
    210 0.85 0.86 0.498 0.495
    240 0.89 0.88 0.477 0.472
    270 0.90 0.89 0.460 0.454
    300 0.90 0.90 0.455 0.451
    下载: 导出CSV

    表  4  串联EFP装药侵彻钢靶仿真计算结果

    Table  4.   Numerical results of tandem EFP charge penetrating the steel target

    b/(mm) Δt/(μs) P/(mm) P/D d/(mm) d/D
    200 10 91.3 1.41 25.8 0.40
    200 20 95.8 1.47 25.2 0.39
    200 25 96.7 1.49 25.0 0.38
    200 30 94.4 1.45 25.9 0.40
    200 40 84.2 1.30 27.7 0.43
    下载: 导出CSV

    表  5  串联EFP装药侵彻钢靶实验结果

    Table  5.   Experimental data of tandem EFP charge penetrating the steel target

    Exp.No. Δt/(μs) P/(mm) P/D d/(mm) d/D
    A1, A2 108 1.661 20 0.308
    B1, B2 10 84 1.292 26 0.400
    B3, B4 20 99 1.523 25 0.385
    B5, B6 25 102 1.569 23 0.354
    B7, B8 30 91 1.400 27 0.415
    B9, B10 40 83 1.277 28 0.431
    下载: 导出CSV
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出版历程
  • 收稿日期:  2012-01-02
  • 修回日期:  2013-09-22

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