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5GPa内JO-9159炸药的磁驱动准等熵压缩响应特性 被引量:10

Response of JO-9159 under Magnetically Driven Quasi-Isentropic Compression to 5 GPa
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摘要 较宽压力范围内未反应炸药的动力学响应特性对于深入认识压缩波作用下炸药起爆热点形成机制具有重要意义。磁驱动准等熵压缩加载(无冲击压缩)是获取较宽压力范围内未反应炸药的动态压缩力学特性的有效手段。基于大电流产生的电磁力作用原理,在国内率先实现了炸药的磁驱动无冲击压缩实验技术,获得了5 GPa内JO-9159炸药在磁驱动准等熵压缩加载下的速度响应历史。利用一维流体动力学编码对加载过程进行了模拟,计算得到的粒子速度曲线与实验测得的粒子速度曲线符合较好。随着厚度的增加,样品与窗口界面处速度的陡度越来越大,加载期间样品应变率峰值在105~106/s量级,随着样品厚度的增加,应变率尖峰变窄、峰值增加。 It is very important and instructive for us to further investigate the formation mechanism of hot spots in explosive initiation in wide pressure zone.Magnetically driven quasi-isentropic compression(shock less compression) is an effective method to research the dynamic behaviors of un-reacted explosives in high pressure.Based on the working principle of electro-magnetic force produced by large current,the shockless compression technique driven by magnetic force is first achieved in domestic.A pressure of 5 GPa is obtained in the experiments of magnetically driven quasi-isentropic compression.The particle velocities of the interface between JO-9159 explosive and LiF windows are gained.The isentropic compression procedure was numerically simulated by one dimensional hydrodynamics code.The simulated particle velocities are in good agreement with experimental results.The gradient of particle velocities between the windows and the samples becomes larger when samples become thicker.The strain ratios of the samples are in 105/s~106/s,and the peak of strain ratio becomes narrower but higher when samples become thicker.
出处 《含能材料》 EI CAS CSCD 北大核心 2011年第5期536-539,共4页 Chinese Journal of Energetic Materials
基金 国家自然科学基金(11002130 10927201) 中物院重点基金(2010A0201006) 双百人才基金(2008R0105)
关键词 固体力学 含能材料 准等熵压缩 动力学响应 solid mechanics energetic materials quasi-isentropic compression dynamic response
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参考文献11

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二级参考文献10

  • 1孙承纬.磁驱动等熵压缩和高速飞片的实验技术[J].爆轰波与冲击波,2005(2):84-92. 被引量:7
  • 2Hare D E. How to Plan and Analyze an Isentropic Compression Experiment (ICE) [R]. UCRL-TR-206486,2004.
  • 3Hall C A,Asay J R, Knudson M D, et al. Experimental Configuration for Isentropic Compression of Solids Using Pulsed Magnetic Loading [J]. Rev Sci Instrum, 2001,72 : 3587.
  • 4Reisman D B,Forbes J W,Tarver C M,et al. Isentropic Compression of LX-04 on the Z Accelerator[A]//Furnish M D,Thadhani N N, Horie Y. Shock Compression of Condensed Matter-2001 [C]. New York: AIP Press, 2002: 849-852.
  • 5Hare D E,Reisman D B,Garcia F,et al,The Isentrope of Unreacted LX-04 to 170 kbar [A]//Furnish M D,Gupta Y M,Forbes J W. Shock Compression of Condensed Matter-2003 [C]. New York:AIP Press, 2004 : 145-148.
  • 6Hooks D E, Hayes D B, Hare D E, et al. Isentropic Compression of Cyclotetramethylene Tetranitramine (HMX) Single Crystals to 50 GPa [J]. J Appl Phys,2006,99:124901.
  • 7Weng J D, Tan H, Hu S L, et al, New All-Fiber Velocimeter [J]. Rev Sci Instrum, 2005,76: 093301.
  • 8Hayes D B. Backward Integration of the Equations of Motion to Correct for Free Surface Perturbations [R]. SAND 2001-1440,2001.
  • 9Wang G J ,Sun C W,Tan F L,et al. The Compact Capacitor Bank CQ-1.5 Employed in Magnetically Driven Isentropic Compression and High Velocity Flyer Plate Experiments [J]. Rev Sci Instrum,2008,79:53904.
  • 10Baer M R, Hall C A,Gustavsen R L, et al. Isentropic Loading Experiments of a Plastic Bonded Explosive and Constituents[J].J Appl Phys, 2007,101 : 034906.

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