Sheftman D, Krasik Y E. Investigation of electrical conductivity and equations of state of non-ideal plasma through underwater electrical wire explosion[J]. Physics of Plasmas, 2010, 112702:1-13.
[2]
Vogel A, Lauterborn W. Acoustic transient generation by laser-produced cavitation bubbles near solid boundaries[J]. Acoust Socam, 1988, 84(2):719-731.
[3]
Tomita Y, Kodama T, Shima A. Secondary cavitation due to interaction of a collapsing bubble with a rising free surface[J]. Appl Phys Lett, 1991, 59(3):274-276..
[4]
Wang Q X, Yeo K S, Khoo B C, et al. Strong interaction between a buyangcy bubble and a free surface[J]. Theoret Comput Fluid Dynamics, 1996, 8:73-88.
[5]
李梅,王树山,马峰.爆炸水幕高度变化规律实验研究[J].北京理工大学学报,2012,32(8):776-780. Li Mei,Wang Shushan,Ma Feng. Experimental research on height variation of explosion plumes[J]. Transactions of Beijing Institute of Technology,2012,32(8):776-780.(in Chinese)
Cole R H. Underwater explosions[M]. New York: Dover Publications INC, 1948.
[8]
Blake J R, Gibson D C. Growth and collapse of a vapour cavity bubble near a free surface[J]. Fluid Mech, 1981, 111:123-140.
[9]
Blake J R, Taib B B, Doherty G. Transient cavities near boundaries Part 2. free surface[J]. J Fluid Mech, 1987, 181:197-212.
[10]
蒋国岩, 金辉, 李兵.水下爆炸研究现状及发展方向展望[J].科技导报, 2009, 27(9):87-91. Jiang Guoyan, Jin Hui, Li Bing. Review of studies on underwater explosion[J]. Science and Technology Review, 2009, 27(9):87-91. (in Chinese)
[11]
Connor J G, Higdon C E. Water barrier line charge plume video analysis[R]. Dahlgren: Naval Surface Warfare Cener, 1996.