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双驱动激波管稀疏波破膜技术研究
引用本文:董志勇,韩肇元.双驱动激波管稀疏波破膜技术研究[J].上海力学,2000,21(4):427-431.
作者姓名:董志勇  韩肇元
作者单位:[1]浙江工业大学建筑工程学院,杭州310014 [2]中国科技大学力学和机械工程系,合肥230026
摘    要:本文介绍了在双驱动激波管中运用稀疏波破膜的技术。在以压缩空气和氮气作实验气体的情形下,实验研究了中间段长度、稀疏波强度及中间段B膜的破膜压力(压差)对第二激波追韩第一激波的影响。实验结果表明:中间段的长短,显著地制约着前后两道激波的间隔;稀疏波强度及中间段B膜的破膜压力对稀疏波破膜时间及第二激小对反射稀疏波的追赶有重要影响。

关 键 词:双驱动激波管  稀疏波  破膜  第一激波  第二激波
修稿时间:2000年4月11日

An Experimental Technique of Diaphragm Burstingby Rarefaction Wave in Double Driver Shock Tube
DONG Zhi-yong,HAN Zhao-yuan.An Experimental Technique of Diaphragm Burstingby Rarefaction Wave in Double Driver Shock Tube[J].Chinese Quarterly Mechanics,2000,21(4):427-431.
Authors:DONG Zhi-yong  HAN Zhao-yuan
Abstract:This paper presents an experimental technique of diaphragm bursting by virtue of the rarefaction wave in double driver shock tube. As far as the compressed air and nitrogen gas are concerned, the effects of length of intermediate section, rarefaction strength and bursting pressure difference across diaphragm on second shock which pursues first shock are experimentally investigated. Experimental results indicate that the interval between two shocks is influenced by the length of intermediate section. The diaphragm opening time due to the rarefaction wave and second shock which pursues reflected rarefaction wave are influenced by the rarefaction strength and breaking pressure difference of diaphragm at the end of intermediate section.
Keywords:double driver shock tube  rarefaction wave  diaphragm bursting  first shock  second shock
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