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694 FENG Song,RAO Guo‑ning,PENG Jin‑hua
ulated by the AUTODYN software. Computed bub‑ of selected cast HMX‑based explosives[J]. Propellants,Explo⁃
ble pulse properties agreed well with measured bub‑ sives,Pyrotechnics,2012,37(2):198-206.
[13] Mader C L.Numerical modeling of explosives and propellants
ble pulse properties for all cases studied,with an av‑
[M]. New York:CRC press,1998:33-52.
erage error of peak pressure of shock wave bubble [14] Levine H B,Sharples R E. Operator's manual for RUBY[R].
period approximately 1.79%,peak pressure 3.70%, UCRL‑6815:1962.
and maximum radius 2.30%. But the numerical re‑ [15] Cowperthwaite M,Zwisler W H. TIGER computer program
sults of bubble images didn't show the light in the documentation[R]. ADA002791:1973.
[16] Nichols A L,Ree F H. CHEQ 2.0 user’s manual[R].UCRL‑MA
bubble. It was different from the experimental imag‑ ‑106754:1990.
es. This simulation work is worth further research. [17] Baker E L,Capellos C,Stiel L I. Jaguar procedures for detona‑
tion properties of aluminized explosives[C]//12th Internation‑
References:
al Detonation Symposium,San Diego,California,2003:333.
[1] Cole R H. Underwater explosions[M]. Princeton:Princeton
[18] Fried L,Howard W M,Souers P C. Cheetah 2.0 user's manu‑
University Press,1948:228-233.
al,lawrence livermore national lab[R]. UCRL‑MA ‑117541 :
[2] Arons A B,Yennie D R. Energy partition in underwater explo‑
1998.
sion phenomena[J]. Reviews of Modern Physics,1948,20
[19] Schoch S,Nikiforakis N. Numerical modelling of underwater
(3):519-536. detonation of non‑ideal condensed‑phase explosives[J]. Phys⁃
[3] Nielsen A T. Caged polynitramine compound:U. S. 5693794 ics of Fluids,2015,27(1):281-288.
[P]. 1997. [20] Donahue L,Zhang F,Ripley R C. Numerical models for after‑
[4] Geetha M,Nair U R,Sarwade D B,et al.Studies on CL‑20:
burning of TNT detonation products in air[J]. Shock Waves,
the most powerful high energy material[J]. Journal of Thermal 2013,23(6):559-573.
Analysis and Calorimetry,2003,73(3):913-922. [21] Wang X,Hossain K,Jackson T L. The three ‑dimensional nu‑
[5] Caulder S M,Buess M L,Nock L A. An analytical study of the merical simulation of aluminized composite solid propellant
crystal quality of ε ‑ Hexanitro ‑ hexaazaisowurtzitane(CL ‑ 20) combustion[J]. Combustion Theory and Modelling,2008,12
synthesized using several different crystallization techniques (1):45-71.
and intermediate precursors[J]. Science and Technology of En⁃ [22] Wang G,Liu G,Peng Q,et al. A SPH implementation with ig‑
ergetic Materials,2005,66(6):406-410. nition and growth and afterburning models for aluminized ex‑
[6] Thangadurai S,Kartha K P S,Sharma D R,et al. Review of plosives[J]. International Journal of Computational Methods,
some newly synthesized high energetic materials[J]. Science 2017,14(04):1750046.
and Technology of Energetic Materials,2004, 65 (6) : [23] Miller P J,Guirguis R H. Effects of late chemical reactions of
215-226. the energy partition in non ‑ ideal underwater explosions[C]//
[7] Nielsen A T,Chafin A P,Christian S L,et al. Synthesis of poly‑ AIP Conference Proceedings,Colorado,1994:309.
azapolycyclic caged polynitramines[J]. Tetrahedron,1998, [24]Miller P J. A reactive flow model with coupled reaction kinetics
54(39):11793-11812. for detonation and combustion in non ‑ ideal explosives[J].
[8] Robidoux P Y,Sunahara G I,Savard K,et al. Acute and MRS Online Proceedings Library Archive,1995,418:413-420
chronic toxicity of the new explosive CL‑20 to the earthworm [25] Abe A,Katayama M,Murata K,et al. Numerical study of un‑
(Eisenia andrei)exposed to amended natural soils[J]. Environ⁃ derwater explosions and following bubble pulses[C]//AIP Con‑
mental Toxicology & Chemistry,2004,23(4):1026-1034. ference Proceedings,Cambridge,2007:955.
[9] Bolton O,Simke L R,Pagoria P F,et al. High power explo‑ [26] Bjarnholt G. Suggestions on standards for measurement and da‑
sive with good sensitivity:A 2:1 cocrystal of CL‑20:HMX[J]. ta evaluation in the underwater explosion test[J].Propellants,
Crystal Growth & Design,2012,12(9):4311-4314. Explosives,Pyrotechnics,1980,5(2-3):67-74.
[10] Simpson R L,Urtiew P A,Ornellas D L,et al. CL‑20 perfor‑ [27] Kowsarinia E,Alizadeh Y,Pour H S S. Experimental evalua‑
mance exceeds that of HMX and its sensitivity is moderate[J]. tion of blast wave parameters in underwater explosion of hexo‑
Propellants,Explosives,Pyrotechnics,1997,22(5):249-255. gen charges[J]. International Journal of Engineering,2012,25
[11] Lewis W K,Rumchik C G,Broughton P B,et al. Time ‑ re‑ (1):65-72.
solved spectroscopic studies of aluminized explosives:chemi‑ [28] Katsabanis P D. Modelling of the underwater shock sensitivity
cal dynamics and apparent temperatures[J]. Journal of Applied of polyurethane FOAM/PETN explosives[J]. Journal of Energet⁃
Physics,2012,111(1):014903. ic Materials,1992,10(4-5):189-220.
[12] Manner V W,Pemberton S J,Gunderson J A,et al. The role [29] Lee J,Kuk J H,Cho Y S,et al. Numerical modeling of under‑
of aluminum in the detonation and post‑detonation expansion water explosion properties for an aluminized explosive[J]. Pro⁃
Chinese Journal of Energetic Materials,Vol.26, No.8 , 2018(686-695) 含能材料 www.energetic-materials.org.cn