期刊文献+

非均匀炸药冲击起爆和起爆后的行为 被引量:2

Behaviors of Shock Initiation and after-Initiation for Heterogeneous Explosives
在线阅读 下载PDF
导出
摘要 介绍并分析了Campbell等人及其他作者研究非均匀炸药冲击起爆和起爆后行为所获得的实验结果,但不涉及其冲击起爆条件。足够强的冲击波进入非均匀炸药后,爆轰将瞬时(指不经过感应时间)且直接(指不经过其他过程,如爆燃)被引发;非均匀炸药起爆后,其中传播的自始至终是一个不断增长的爆轰波,直至发展为正常爆轰,整个过程都是爆轰的增长(新定义)过程。不存在由反应冲击波不断增长并转变为爆轰波的所谓向爆轰的增长。所谓向爆轰的增长,实际上是爆轰的增长(按新定义)的初期;Craig原定义的爆轰的增长,实际上是爆轰的增长(按新定义)的后期;而所谓反应冲击波,实际上是增长中的初期爆轰波。爆轰的增长(按新定义)是所有猛炸药的特性,炸药反应不充分并逐渐趋于充分是爆轰的增长的化学机制。 Campbell's and other authors' experimental studies of behaviors of initiation and after-ruination for heterogeneous explosives were introduced and analyzed,but initiation conditions were not dealt with. When an intense shock wave enters a heterogeneous explosive charge, detonation is initiated by the shock wave instantaneously (i. e. not to undergo induction time) and directly (i. e. ,not to pass through other processes, such as deflagration). Then a building up detonation wave propagates throughout the heterogeneous explosive charge until it develops into a normal detonation. This whole process is called the buildup of detonation with the new definition in this paper. The so-called reactive shock wave is the building up detonation wave in early stage. Buildup of detonation (in terms of new definition) is a characteristic for all secondary explosives, incomplete reaction and running to complete reaction of explosives are the chemical mechanism of buildup of detonation.
作者 李银成
出处 《高压物理学报》 EI CAS CSCD 北大核心 2006年第1期102-108,共7页 Chinese Journal of High Pressure Physics
关键词 炸药 爆轰 起爆 explosive detonation initiation equation of state
  • 相关文献

参考文献15

  • 1李银成.均匀炸药冲击起爆和起爆后的行为[J].高压物理学报,2005,19(3):247-256. 被引量:4
  • 2Campbell A W,Davis W C,Travis J R.Shock Initiation of Detonation in Liquid Explosives[J].Physics of Fluids,1961,4(4):498-510.
  • 3Campbell A W,Davis W C,Ramsay J B,et al.Shock Initiation of Solid Explosives[J].Physics of Fluids,1961,4(4):511-521.
  • 4Majowicz J M,Jacobs S J.Bull Am Phys Soc,1958,5:293.
  • 5Lindstrom I E.Plane Shock Initiation of an RDX Plastic-Bonded Explosive[J].J Appl Phys,1966,37(13):4873-4880.
  • 6Lindstrom I E.Plane Shock Initiation of Porous Tetryl[J].J Appl Phys,1970,41(1):337-350.
  • 7Stirpe D,Johnson J O,Wackerle J.Shock Initiation of XTX-8003 and Pressed PETN[J].J Appl Phys,1970,41(9):3884-3893.
  • 8Dick J J.Buildup to Detonation in Solid High Explosives during Plane Shock Initiation[A].//18th Symposium(International) on Combustion[C].1981:1623-1629.
  • 9Mader C L.Numerical Modeling of Detonation[M].Berkeley,California:University of California Press,1979:106-115;125-130.
  • 10Dobratg B M.Properties of Chemical Explosives and Explosives Simulants[R].UCRL-52997,1981.

二级参考文献21

  • 1李银成.爆轰产物的冷比内能与冷压的函数表达式[J].高压物理学报,2005,19(1):71-79. 被引量:1
  • 2丁--,北京理工大学学报,1986年,1期
  • 3刘家聪,爆炸与冲击,1984年,4卷,3期,31页
  • 4吴国栋,1983年
  • 5李维新,爆炸与冲击,1983年,3卷,2期,30页
  • 6Trevino S F,Tai D H. Simulation of the Initiation of Detonation in an Energetic Molecular Crystal [A]. 8th Symposium on Detonation [C]. 1985. 870-880.
  • 7崔季平 何宇中.晶格能量弛豫与激波作用下凝聚态分子的稳定性[A]..第四届全国爆轰学术会议论文集(下)[C].山海关,1994.1-2.
  • 8Campbell A W,Davis W C,Travis J R. Shock Initiation of Detonation in Liquid Explosives [J]. Phys Fluids,1961,4(4):498-510.
  • 9Hubbard H W,Johnson M H. Initiation of Detonations [J]. J Appl Phys,1959,30:765.
  • 10Campbell A W,Davis W C,Ramsay J B,et al. Shock Initiation of Solid Explosives [J]. Phys Fluids,1961,4(4) :511-521.

共引文献3

同被引文献54

引证文献2

二级引证文献8

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部