狭长直管约束条件水下电爆炸所产生的气泡运动和界面射流  被引量:4

Bubble and jet induced by underwater wire explosion in a narrow tube

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作  者:张桂夫[1] 朱雨建[1] 李元超[1] 杨基明[1] 

机构地区:[1]中国科学技术大学近代力学系,安徽合肥230026

出  处:《爆炸与冲击》2015年第5期609-616,共8页Explosion and Shock Waves

基  金:国家自然科学基金项目(11102204)

摘  要:以高速摄影为主要手段,揭示直管中爆炸诱导气泡和射流的典型演变过程,并测试爆炸深度和爆炸能量对该现象的影响。研究发现直管中爆炸诱导的表面射流分为光滑和粗糙的两段,这区别于自由表面射流的形态;爆炸气泡的发展经历一个先膨胀再坍缩的过程,其中封闭坍缩以气泡顶部形成内向射流为特征。表面射流速度主要来自爆炸早期短时间内气泡膨胀赋予水体的冲量,且整体上与起爆能量成正相关,而与爆炸深度成反相关;用准一维的简化模型能够很好地描述它们之间的依赖关系,计算结果不仅在趋势上与实验结果一致,数值上也能很好吻合。A high-speed video camera was employed to record the flow field directly. Different explo- sion energy (discharging voltage) and explosion depth were examined. It is found that the surface jet formed in the narrow tube consists of a smooth upper body and a rough root, which differs from the general recognition of free surface jets. The bubble induced by the wire explosion underwent an ex- pansion-collapse process, and the close-in collapse was characterized by a downward inner jet popping out from the bubble roof. The study also reveals that the strength of the surface jet increases with the explosion energy while decreases with explosion depth. A quasi-one-dimensional theoretical model was proposed to analyze the parametric dependences. It turns out not only the variation trend but also the exact value of both maximum bubble scale and jet velocity can be well predicted by this model.

关 键 词:爆炸力学 射流 水下电爆炸 狭长直管 气泡 

分 类 号:O381[理学—流体力学]

 

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