新型乳化炸药动压减敏装置的数值模拟研究

程扬帆 汪泉 缪广红 沈兆武 颜事龙

程扬帆, 汪泉, 缪广红, 沈兆武, 颜事龙. 新型乳化炸药动压减敏装置的数值模拟研究[J]. 高压物理学报, 2016, 30(4): 311-316. doi: 10.11858/gywlxb.2016.04.007
引用本文: 程扬帆, 汪泉, 缪广红, 沈兆武, 颜事龙. 新型乳化炸药动压减敏装置的数值模拟研究[J]. 高压物理学报, 2016, 30(4): 311-316. doi: 10.11858/gywlxb.2016.04.007
CHENG Yang-Fan, WANG Quan, MIAO Guang-Hong, SHEN Zhao-Wu, YAN Shi-Long. Numerical Simulation on a Novel Dynamic Pressure Desensitization Device for Emulsion Explosives[J]. Chinese Journal of High Pressure Physics, 2016, 30(4): 311-316. doi: 10.11858/gywlxb.2016.04.007
Citation: CHENG Yang-Fan, WANG Quan, MIAO Guang-Hong, SHEN Zhao-Wu, YAN Shi-Long. Numerical Simulation on a Novel Dynamic Pressure Desensitization Device for Emulsion Explosives[J]. Chinese Journal of High Pressure Physics, 2016, 30(4): 311-316. doi: 10.11858/gywlxb.2016.04.007

新型乳化炸药动压减敏装置的数值模拟研究

doi: 10.11858/gywlxb.2016.04.007
基金项目: 

国家自然科学基金 51374189

国家自然科学基金 11502001

安徽省高等学校自然科学研究项目 KJ2015A074

安徽省自然科学基金 1608085QA15

详细信息
    作者简介:

    程扬帆(1987—), 男,讲师,主要从事含能材料的实验和数值模拟研究.E-mail:cyf518@mail.ustc.edu.cn

  • 中图分类号: O389

Numerical Simulation on a Novel Dynamic Pressure Desensitization Device for Emulsion Explosives

  • 摘要: 利用LS-DYNA动力学有限元软件,对新型乳化炸药动压减敏装置的作用过程进行了三维数值模拟,研究了该装置在水下爆炸过程中的流场分布特征,及其结构设计对实验结果的影响。对比研究结果表明,新型乳化炸药动压减敏装置中, 受压乳化炸药之间的排距是影响实验精度的关键因素,当乳化炸药的半径为2cm、主发药RDX的质量为10g时,乳化炸药的最小排距(即前排乳化炸药对后排乳化炸药影响最小时的排距)为20cm。因此,在乳化炸药动态减敏实验开展之前,可以通过数值模拟的手段预先确定最小排距,减小实验误差。该方法可为乳化炸药动压减敏的后续深入研究提供参考。

     

  • 图  传统的冲击波动压减敏实验原理图

    Figure  1.  Schematic of traditional dynamicpressure desensitization experiment

    图  改进后的冲击波动压减敏实验原理图

    Figure  2.  Schematic of improved dynamicpressure desensitization experiment

    图  三维计算模型

    Figure  3.  Three-dimensional calculation model

    图  不同时刻(t)新型动压减敏装置的流场分布特征图

    Figure  4.  Flow field distribution of new dynamic pressure desensitization device at different time

    图  若干临界位置处冲击波压力时程曲线与无阻挡情况的比较

    Figure  5.  Comparison of shock wave pressure-history at several critical positions with unblocked condition

    图  乳化炸药后不同位置处冲击波的压力时程曲线与无阻挡情况的比较

    Figure  6.  Comparison of shock wave pressure-history at several positions behind the emulsion explosive with unblocked condition

    表  1  水的Mie-Grüneisen状态方程参数

    Table  1.   State parameters of Mie-Grüneisen equation for water

    C/(m/s) S1 S2 S3 γ0 a
    1480 1.92 0 0 0.35 0
    下载: 导出CSV

    表  2  乳化炸药的阻挡对若干临界位置处冲击波压力的影响

    Table  2.   The influence of emulsion explosive on the shock wave at several critical positions

    Spacing from theRDX/(cm) Peak pressure/(MPa) Influencing degree/(%)
    With a block Without a block
    24 77.6 77.6 0
    26 44.1 47.5 7.2
    50 23.1 23.2 0.4
    下载: 导出CSV

    表  3  前排乳化炸药的阻挡对其后不同位置处冲击波压力的影响

    Table  3.   The influence of emulsion explosive of front row on the shock wave at different following positions

    Spacing from emulsion explosiveof the 1st row/(cm) Peak pressure/(MPa) Influencing degree/(%)
    With a block Without a block
    10 35.5 36.5 2.7
    15 31.6 31.8 0.6
    20 27.0 27.1 0.4
    25 23.1 23.2 0.4
    下载: 导出CSV
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出版历程
  • 收稿日期:  2015-05-18
  • 修回日期:  2015-07-08

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