Experimental study on initiated reaction evolution of pressed explosives in long thick wall cylinder confinement

被引:0
作者
Qiu T. [1 ,2 ]
Wen S. [2 ]
Li T. [3 ]
Hu H. [3 ]
Fu H. [3 ]
Shang H. [3 ]
机构
[1] CAS Key Laboratory of Mechanical Behavior and Design of Materials (LMBD) Department of Modern Mechanics University of Science and Technology of China, Hefei, 230026, Anhui
[2] Institute of Chemical Materials, CAEP, Mianyang, 621999, Sichuan
[3] Laboratory for Shock Wave and Detonation Physics Research, Institute of Fluid Physics, CAEP, Mianyang, 621999, Sichuan
来源
Baozha Yu Chongji/Explosion and Shock Waves | 2020年 / 40卷 / 01期
关键词
Convective flow; DDT; Laminar burning; Pressed PBX;
D O I
10.11883/bzycj-2019-0360
中图分类号
学科分类号
摘要
In order to investigate whether the reaction evolution of pressed HMX-based PBXs inside long thick wall steel tube initiated by ignition composition leads to detonation finally or not, a new experiment apparatus was designed based on traditional DDT tube, in which the strength of tube at specific locations is enhanced, and multichannel PDV probes and high speed photography were used to diagnose the expansion process and rupture characteristics of tube wall. Compared with the results initiated by detonator in the same explosives and confinement, the reaction durations of detonation and ignition differed by orders of magnitude; the pressure evolution measured by tube wall velocities, and the propagation process of tube wall movement were significantly different in two reactions. Analysis shows that the convective flow of reaction products along the seam between tube wall and explosives, high temperature and pressure, dominated the reaction evolution of PBX-A initiated by ignition composition under strong confinement, and appeared as laminar burning on explosive surface and structural response of confinement. There is no reaction activated in explosive bulk by the ramp wave caused by upper stream non shock initiation reaction, least of all DDT. © 2020, Editorial Staff of EXPLOSION AND SHOCK WAVES. All right reserved.
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相关论文
共 17 条
[1]  
Asay B., Shock Wave Science and Technology Reference Library, Non-shock Initiation of Explosives, 5, pp. 11-488, (2010)
[2]  
Macek A., Transition from deflagration to detonation in cast explosive, Journal of Chemical Physics, 31, 1, pp. 162-167, (1959)
[3]  
Tarver C.M., Goodale T.C., Shaw R., Et al., Deflagration-to-detonation transition studiesfor two potential isomeric cast primary explosives, 6th Symposium(International) on Detonation, pp. 231-249, (1976)
[4]  
Jacobs S., Personal communication with C. M. Tarver., 6th Symposium (International) on Detonation, (1976)
[5]  
Bernecker R.R., Sandusky H.W., Clairmont A.R., Deflagration-to-detonation transition studies of porous explosivecharges in plastic tubes, Proceeding of the 7th Symposium (International) on Detonation, pp. 119-138, (1981)
[6]  
Sandusky H.W., Bernecker R.R., Compressive reaction in porous beds of energetic materials, 8th Symposium (International) on Detonation, pp. 881-891, (1985)
[7]  
Campbell A.W., Deflagration-to-detonation in granular HMX: LA-UR 80-2016, (1980)
[8]  
Zhang T.H., Bai Y.L., Wang S.Y., Et al., Deflagration-to-detonationtransition in porous propellants and cast propellants, Explosion and Shock Waves, 20, 4, pp. 296-302, (2000)
[9]  
Zhao T.H., Zhang X.Y., Li B., Et al., Experimental study on the deflagration-to-detonation transition for granular HMX, RDX, Chinese Journal of Energetic Materials, 11, 4, pp. 187-190, (2003)
[10]  
Maienschein J.L., Chandler J.B., Burn rates of pristine and degraded explosives at elevated temperatures and pressures: UCRL-JC-127993, (1998)