供风量与气泡帷幕层数协同下水中爆炸冲击波的削波效果

杜明燃 陈智凡 陆少锋 梁进 李基锐 王尹军 王天照 陈宇航

杜明燃, 陈智凡, 陆少锋, 梁进, 李基锐, 王尹军, 王天照, 陈宇航. 供风量与气泡帷幕层数协同下水中爆炸冲击波的削波效果[J]. 高压物理学报, 2024, 38(1): 015103. doi: 10.11858/gywlxb.20230705
引用本文: 杜明燃, 陈智凡, 陆少锋, 梁进, 李基锐, 王尹军, 王天照, 陈宇航. 供风量与气泡帷幕层数协同下水中爆炸冲击波的削波效果[J]. 高压物理学报, 2024, 38(1): 015103. doi: 10.11858/gywlxb.20230705
DU Mingran, CHEN Zhifan, LU Shaofeng, LIANG Jin, LI Jirui, WANG Yinjun, WANG Tianzhao, CHEN Yuhang. Synergistic Effect of Air Supply Volume and Bubble Curtain Layer on the Shock Wave Attenuation of Underwater Explosion[J]. Chinese Journal of High Pressure Physics, 2024, 38(1): 015103. doi: 10.11858/gywlxb.20230705
Citation: DU Mingran, CHEN Zhifan, LU Shaofeng, LIANG Jin, LI Jirui, WANG Yinjun, WANG Tianzhao, CHEN Yuhang. Synergistic Effect of Air Supply Volume and Bubble Curtain Layer on the Shock Wave Attenuation of Underwater Explosion[J]. Chinese Journal of High Pressure Physics, 2024, 38(1): 015103. doi: 10.11858/gywlxb.20230705

供风量与气泡帷幕层数协同下水中爆炸冲击波的削波效果

doi: 10.11858/gywlxb.20230705
基金项目: 安徽省高校科学研究项目(KJ2021A0431);广西重点研发计划(桂科AB22035001);安徽省自然科学基金(1908085QA33);安徽理工大学引进人才科研启动基金(11881);广西重点研发计划(防科AB21014001)
详细信息
    作者简介:

    杜明燃(1987-),男,博士,副教授,主要从事炸药性能和爆破技术研究. E-mail:dumingranaust@163.com

    通讯作者:

    陈智凡(1999-),男,硕士研究生,主要从事水中爆炸研究. E-mail:786923403@qq.com

  • 中图分类号: O389; TD235

Synergistic Effect of Air Supply Volume and Bubble Curtain Layer on the Shock Wave Attenuation of Underwater Explosion

  • 摘要: 气泡帷幕能有效地削弱水中冲击波对周围环境的影响。为了研究气泡帷幕供风量和层数对水中冲击波的协同作用,在供风量为30、60、90 L/min的条件下分别设计了含1、2、3层气泡帷幕的水下爆炸试验。结果表明,气泡帷幕的衰减率随供风量和层数增加而增大。当供风量较小(如30、60 L/min)时,随着气泡帷幕层数的增加,相邻层数之间峰值压力的衰减效率越来越低;当供风量较大(如90 L/min)时,随着气泡帷幕层数的增加,相邻层数之间峰值压力的衰减效率越来越高。结合实际工程的经济效益和水下复杂环境问题对削波效果进行分析,确定在供风量为30 L/min时开启2层气泡帷幕是最优的削波方案,为相关的实际工程问题提供参考和新思路。

     

  • 图  气泡帷幕发生器

    Figure  1.  Bubble curtain generator

    图  现场试验中气泡帷幕发生器的作用效果

    Figure  2.  Effect of bubble curtain generator in field test

    图  现场布置示意图

    Figure  3.  Schematic diagram of test arrangement

    图  空白对照组的冲击波压力时程曲线

    Figure  4.  Time histories of shock wave pressure in blank control group

    图  供风量为30、60、90 L/min时的冲击波压力时程曲线

    Figure  5.  Time histories of shock wave pressure with air supply volume of 30,60 and 90 L/min

    图  供风量为30 L/min、不同气泡帷幕层数时的冲击波压力时程曲线

    Figure  6.  Time histories of shock wave pressure under different layers of bubble curtains with the air supply volume of 30 L/min

    图  相邻层数之间的衰减效率Bi

    Figure  7.  Attenuation efficiency Bi between adjacent layers

    图  相邻梯度供风量之间的衰减效率Cj

    Figure  8.  Attenuation efficiency Cj between adjacent air supply volumes

    表  1  试验设计方案

    Table  1.   Design scheme of field test

    Test No. v/(L·min−1) n Test No. v/(L·min−1) n Test No. v/(L·min−1) n
    1 0 0 8 90 1 15 30 3
    2 0 0 9 30 2 16 30 3
    3 30 1 10 30 2 17 60 3
    4 30 1 11 60 2 18 60 3
    5 60 1 12 60 2 19 90 3
    6 60 1 13 90 2 20 90 3
    7 90 1 14 90 2
    下载: 导出CSV

    表  2  不同层数气泡帷幕条件下水下冲击波峰值压力

    Table  2.   Peak pressure of underwater explosion shock wave under different layers of bubble curtains

    v/(L·min−1) n=1 n=2 n=3
    pm/MPa $ {\overline{p}}_{\mathrm{m}}/{\mathrm{MPa}} $ A/% pm/MPa $ {\overline{p}}_{\mathrm{m}}/{\mathrm{MPa}} $ A/% pm/MPa $ {\overline{p}}_{\mathrm{m}} /{\mathrm{MPa}}$ A/%
    30 2.069
    1.991
    2.030 49.67 0.931
    0.944
    0.938 76.74 0.831
    0.870
    0.851 78.90
    60 1.547
    1.501
    1.524 62.21 0.842
    0.801
    0.822 79.62 0.633
    0.681
    0.657 83.71
    90 0.760
    0.796
    0.778 80.71 0.655
    0.684
    0.670 83.39 0.390
    0.392
    0.391 90.30
    下载: 导出CSV
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出版历程
  • 收稿日期:  2023-08-08
  • 修回日期:  2023-09-14
  • 网络出版日期:  2024-01-29
  • 刊出日期:  2024-02-05

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