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张阿漫 王诗平 白兆宏 黄超. 不同环境下气泡脉动特性实验研究[J]. 力学学报, 2011, 43(1): 71-83. DOI:10.6052/0459-1879-2011-1-lxxb2010-278
引用本文: 张阿漫 王诗平 白兆宏 黄超. 不同环境下气泡脉动特性实验研究[J]. 力学学报, 2011, 43(1): 71-83.DOI:10.6052/0459-1879-2011-1-lxxb2010-278
zhang Aman Wang Shiping Bai Zhaohong Chao HUANG. Experimental study on bubble pulse features under different circumstances[J]. Chinese Journal of Theoretical and Applied Mechanics, 2011, 43(1): 71-83. DOI:10.6052/0459-1879-2011-1-lxxb2010-278
Citation: zhang Aman Wang Shiping Bai Zhaohong Chao HUANG. Experimental study on bubble pulse features under different circumstances[J].Chinese Journal of Theoretical and Applied Mechanics, 2011, 43(1): 71-83.DOI:10.6052/0459-1879-2011-1-lxxb2010-278

不同环境下气泡脉动特性实验研究

Experimental study on bubble pulse features under different circumstances

  • 摘要:水下爆炸气泡对舰船结构造成严重的毁伤, 海上实船爆炸实验是考核水下爆炸气泡对舰船毁伤威力最直接、最有效的方法, 然而真实情况的舰船水下爆炸实验难以进行.为此, 在已有研究成果的基础上, 设计实验电路, 利用电容在相对较低的电压下放电打火产生的电火花气泡来模拟水下爆炸气泡, 设计多组实验工况来模拟气泡在不同环境下的运动特性. 研究气泡在不同环境下的脉动特性、射流特征, 揭示一些特殊的实验现象, 总结环境对气泡运动的影响规律.

    Abstract:Underwater explosion bubbles do severe damage to warshipstructures, and the particularity of underwater explosion and the quality ofwater bring great difficulties to get a clear picture. So lots oflaboratories all around the world make use of discharge or laser to generatebubbles to replace real underwater explosion experiments.Based on the designation from Turangan et al and Abdolranman Dadvand, anelectric circuit with a relatively low voltage 200V and three shunt-wound2200\muF capacitances is used to generate bubbles by discharge ina 500mm\times500mm\times500mm water tank to study underwater bubbledynamics. The experiment setup is safe, stable, low in costs and simple tofix. It can generate bubbles with radius up to 12~15mm.A device generating bubble by a relatively low voltage is designed to studybubble dynamics in detail under various boundary conditions in this paper.Main conclusions are obtained below by comparison and analysis:(1) A voltage of 200 V is adopted to generate bubble by discharge in water inthis paper. The voltage is fairly low yet the bubble generated is relativelylarge in size. The pictures shot are pretty clear as well.(2) There are copper wires burning inside the bubble throughout theexpansion process, causing the temperature inside bubble to rise apparentlyhigher and result in the small calculated value of bubble pulsing period. Sop_v within the bubble is actually very large and the calculated p_v ofa single bubble pulsing in free field is 5.8\times 10^4 Pa.(3) Bubble's second pulsing energy is merely 5\%\sim 15\% of the firstpulsing energy and the pulsing energy after the second pulse can be ignored.(4) \gamma , the dimensionless standoff is defined betweenbubble and boundary. When \gamma \ge 2.8, the influence of the wall tobubble can be neglected. When 1.95 \le \gamma \le 2.8, no jet is formedduring the first cycle of bubble pulse. When \gamma \le 1.53, jet is formedduring the first cycle of bubble pulse, and the smaller \gamma is, thelarger bubble migration distance and the more fiercely the jet would be.(5) The bubble jetting velocity is minimum when the dimensionless standoff\gamma is around 0.8.(6) Bubble will interact strongly with boundaries when it moves near theshipboard and the free surface. It can be seen from the experiments that thebubble may produce jets that are towards two different directions whencollapsing near the free surface and the shipboard, and this will certainlylead to the weakening effect of bubble attack to the shipboard.

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