Experimental investigation of the reaction-build-up for plastic bonded explosive JOB-9003

Zhang Xu; Wang Yanfei; Zhao Feng; Zhang Rong; Zhong Bin

doi:10.1016/j.mre.2017.02.001

Volume 2 Issue 3

May 2017

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Zhang Xu, Wang Yanfei, Zhao Feng, Zhang Rong, Zhong Bin. Experimental investigation of the reaction-build-up for plastic bonded explosive JOB-9003[J]. Matter and Radiation at Extremes, 2017, 2(3). doi: 10.1016/j.mre.2017.02.001

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Zhang Xu, Wang Yanfei, Zhao Feng, Zhang Rong, Zhong Bin. Experimental investigation of the reaction-build-up for plastic bonded explosive JOB-9003[J]. Matter and Radiation at Extremes, 2017, 2(3). doi: 10.1016/j.mre.2017.02.001

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Experimental investigation of the reaction-build-up for plastic bonded explosive JOB-9003

doi: 10.1016/j.mre.2017.02.001

1.
aNational Laboratory of Shock Wave and Detonation Physics, Institute of Fluid Physics, China Academy of Engineering Physics, Mianyang, Sichuan, 621900, China
2.
bGraduate School of China Academy of Engineering Physics, Mianyang, Sichuan, 621900, China

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Corresponding author: *Corresponding author. E-mail address: caepzx@sohu.com (X. Zhang).
Received Date: 2016-02-17
Accepted Date: 2016-09-14
Publish Date: 2017-05-15

Abstract

Abstract

In order to measure the shock initiation behavior of JOB-9003 explosives, Al-based embedded multiple electromagnetic particle velocity gauge technique has been developed. In addition, a gauge element called the shock tracker has been used to monitor the progress of the shock front as a function of time, thus providing a position–time trajectory of the wave front as it moves through the explosive sample. The data is used to determine the position and time for shock to detonation transition. All the experimental results show that the rising-up time of Al-based electromagnetic particle velocity gauge is very short (<20 ns); the reaction-build-up velocity profiles and the position–time for shock to detonation transition of HMX-based plastic bonded explosive (PBX) JOB-9003 with 1–8 mm depth from the origin of the impact plane under different initiation pressures were obtained with high accuracy.
- Embedded electromagnetic particle velocity gauge,
- JOB-9003 explosive,
- Particle velocity profile

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References(41)

References

[1]	V.M. Zaitzev, P.F. Pokhil, K.K. Shvedov, The Electromagnetic Method for the Measurements of Velocities of Detonation Products, DAN SSSR 132 1339, 1960.
[2]	J.E. Vorthman, Facilities for the study of shock induced decomposition of high explosives, in: L. Seaman, R.A. Graham (Eds.), Shock Waves in Condensed Matter, American Institute of Physics, New York, 1981, p. 680.
[3]	J. Vorthman, G. Andrews, J. Wackerle, Reaction rates from electromagnetic gauge data, in: J.M. Short (Ed.), Proc. 8th Symp. (Int.) on Detonation, Naval Surface Weapons Center, Silver Spring, MD, 1980, pp. 99–110.
[4]	L.M. Erickson, W.L. Parker, H.C. Vantine, K.C. Weingart, R.S. Lee, The electromagnetic velocity gauge: use of multiple gauges, time response, and flow perturbations, in: J.M. Short (Ed.), Proc. 7th Symp. (Int.) on Detonation, Naval Surface Weapons Center, Dahlgren, VA, 1981, pp. 1062–1071.
[5]	Y.M. Gupta, D.D. Keough, D.F. Walter, K.C. Dao, D. Henley, A. Urweider, Experimental facility to produce and measure compression and shear waves in impacted solids, Rev. Sci. Instrum. 51 (1980) 183–194.10.1063/1.1136171
[6]	R. Fowles, R.F. Williams, Plane wave stress propagation in solids, J. Appl. Phys. 41 (1) (1970) 360–365.10.1063/1.1658348
[7]	A.W. Campbell, W.C. Davis, J.B. Ramsay, F.R. Travis, Shock initiation of solid explosive, Phys. Fluids 21 (4) (1961) 511–577.10.1063/1.1706354
[8]	J.J. Dick, C.A. Forest, J.B. Ramsay, W.L. Seitz, The Hugoniot and shock sensitivity of a plastic-bonded TATB explosive PBX 9502, J. Appl. Phys. 63 (1988) 4881–4887.10.1063/1.340428
[9]	R.L. Gustavsen, S.A. Sheffield, R.R. Alcon, Measurements of shock initiation in the tri-amino-tri-nitro-benzene based explosive PBX 9502: wave forms from embedded gauges and comparison of four different material lots, J. Appl. Phys. 99 (2006) 114907.10.1063/1.2195191
[10]	R.L. Gustavsen, S.A. Sheffield, R.R. Alcon, Low pressure shock initiation of porous HMX for two grain size distributions and two densities, in: American Institute of Physics (AlP) Conference Proceedings, 1995.
[11]	S.A. Sheffield, R.R. Alcon, R.L. Gustavsen, R.A. Graham, M.U. Anderson, Particle velocity and stress measurements in low density HMX, in: S.C. Schmidt, J.W. Shaner, G.A. Samara, M. Ross (Eds.), American Institute of Physics (AlP) Conference Proceedings, 1993.
[12]	R.L. Gustavsen, S.A. Sheffield, Double shock initiation of the HMX based explosive EDC-37, in: AlP Conference Proceedings, 2002.
[13]	S.A. Sheffield, R.L. Gustavsen, R.R. Alcon, In-situ magnetic gauging technique used at LANL-method and shock information obtained, in: M.D. Furnish, L.C. Chhabildas, R.S. Hixson (Eds.), Shock Compression of Condensed Matter, 1999, American Institute of Physics, New York, 2000, pp. 1043–1050.
[14]	R.R. Alcon, R.N. Mulford, Shock tracker configuration of in-material gauge, in: S.C. Schmidt, W.C. Tao (Eds.), Shock Compression of Condensed Matter 1995, American Institute of Physics, New York, 1996, pp. 1057–1060.
[15]	R.R. Alcon, S.A. Sheffield, A.R. Martinez, R.L. Gustavsen, Magnetic gauge instrumentation on the LANL gas-driven two-stage gun, in: S.C. Schmidt, D.P. Dandekar, J.W. Forbes (Eds.), Shock Compression of Condensed Matter 1997, 1998.
[16]	R.L. Gustavsen, S.A. Sheffield, R.R. Alcon, Low pressure shock initiation of porous HMX for two grain size distributions and two densities, in: S.C. Schmidt, W.C. Tao (Eds.), Shock Compression of Condensed Matter 1995, American Institute of Physics, New York, 1996, pp. 851–854.
[17]	R.L. Gustavsen, S.A. Sheffield, R.R. Alcon, Detonation wave profiles in HMX based explosives, in: S.C. Schmidt, D.P. Dandekar, J.W. Forbes (Eds.), Shock Compression of Condensed Matter 1997, American Institute of Physics, New York, 1998, pp. 739–742.
[18]	R.L. Gustavsen, S.A. Sheffield, R.R. Alcon, L.G. Hill, R.E. Winter, et al., Initiation of EDC-37 measured with embedded electromagnetic particle velocity gauges, in: M.D. Furnish, L.C. Chhabildas, R.S. Hixson (Eds.), Shock Compression of Condensed Matter, 1999, American Institute of Physics, New York, 2000, pp. 879–882.
[19]	W.F. Hemsing, Velocity sensing interferometer (VISAR) modification, Rev. Sci. Instrum. 50 (1) (1979) 73–78.10.1063/1.1135672
[20]	E. Barsis, E. Williams, C. Skoog, Piezoresistivity coefficients in manganin, J. Appl. Phys. 41 (1980) 5155–5162.10.1063/1.1658638
[21]	S.C. Gupta, Y.M. Gupta, Piezoresistive response of longitudinally and laterally orientated ytterbium foils subjected to impact and quasi-static loading, J. Appl. Phys. 57 (1986) 2464–2473.10.1063/1.335430
[22]	Z. Rosenberg, Y. Partom, Lateral stress measurement in shock-loaded targets with transverse piezoresistive gauges, J. Appl. Phys. 58 (1985) 3072–3076.10.1063/1.335833
[23]	J.C. Millett, N.K. Bourne, Z. Rosenberg, On the analysis of transverse stresses during shock loading experiments, J. Phys. D: Appl. Phys. 29 (1996) 2466–2472.10.1088/0022-3727/29/9/035
[24]	J.A. Charest, C.S. Lynch, The response of PVF2 stress gauges to shock wave loading, in: S.C. Schmidt, J.N. Johnson, L.W. Davidson (Eds.), Shock Compression of Condensed Matter 1989, Elsevier, Amsterdam, 1990, pp. 797–800.
[25]	J.A. Charest, C.S. Lynch, A simple approach to piezofilm stress gauges, in: S.C. Schmidt et al. (Ed.), Shock Compression of Condensed Matter 1991, North-Holland, Amsterdam, 1992, pp. 897–900.
[26]	D.B. Hayes, Polymorphic phase transformation in shock-loaded potassium chloride, J. Appl. Phys. 45 (1974) 1208–1217.10.1063/1.1663391
[27]	Z. Rosenberg, D. Yaziv, Y. Partom, Direct measurement of strain in plane impact experiments by a longitudinal resistance gauge, J. Appl. Phys. 51 (1980) 4790–4798.10.1063/1.328311
[28]	R.N. Mulford, R.R. Alcon, Shock initiation of PBX-9502 at elevated temperatures, in: S.C. Schmidt, W.C. Tao (Eds.), Shock Compression of Condensed Matter 1995, American Institute of Physics, New York, 1996, pp. 855–858.
[29]	S.A. Sheffield, R.L. Gustavsen, R.R. Alcon, Observations of shock-induced reaction in liquid bromoform up to 11 GPa, in: S.C. Schmidt, W.C. Tao (Eds.), Shock Compression of Condensed Matter 1995, American Institute of Physics, New York, 1996, pp. 771–774.
[30]	S.A. Sheffield, R.L. Gustavsen, R.R. Alcon, Hugoniot and initiation measurements on TNAZ explosive, in: S.C. Schmidt, W.C. Tao (Eds.), Shock Compression of Condensed Matter 1995, American Institute of Physics, New York, 1996, pp. 879–882.
[31]	S.A. Sheffield, R.L. Gustavsen, R.R. Alcon, Porous HMX initiation studies—sugar as an inert simulant, in: S.C. Schmidt, D.P. Dandekar, J.W. Forbes (Eds.), Shock Compression of Condensed Matter 1997, American Institute of Physics, New York, 1998, pp. 575–578.
[32]	L.L. Davis, S.A. Sheffield, R. Engelke, Detonation properties of bromonitromethane, in: M.D. Furnish, L.C. Chhabildas, R.S. Hixson (Eds.), Shock Compression of Condensed Matter 1999, American Institute of Physics, New York, 2000, pp. 785–788.
[33]	J.J. Dick, Stress–strain response of PBX 9501 below 1 gigapascal from embedded magnetic gauge data using Lagrangian analysis, in: M.D. Furnish, L.C. Chhabildas, R.S. Hixson (Eds.), Shock Compression of Condensed Matter, American Institute of Physics, New York, 2000, pp. 683–686.
[34]	L.J. Wen, Z.P. Duan, Z.Y. Zhang, F.L. Huang, Experimental study build-up difference of HMX and TATB based PBX explosive, Explos. Shock Wave 26–32 (2013).
[35]	Z.P. Li, X.P. Long, Y.M. Huang, B. He, et al., Experimental method and application of electromagnetic particle velocity technique, Energy Mater. 13 (6) (2005) 359–361.
[36]	Z.P. Li, X.P. Long, Y.M. Huang, B. He, et al., Initiation of JOB-9003 explosive study with electromagnetic particle velocity technique, Explos. Shock Wave 26 (3) (2006) 269–272.
[37]	S.P. Wang, Study of electromagnetic particle velocity technique, Det. Shock Wave 4 (1) (1985) 33–35.
[38]	C. Yu, Shock Hugoniot relation of JB-9001 high explosive, Chin. J. High Press. Phys. 12 (1) (1998) 72–77.
[40]	M.B. Boslough, T.J. Ahrens, Particle velocity experiments in anorthosite and gabbro, Amsterdam: North-Holland, in: J.R. Asay, R.A. Graham, G.K. Straub (Eds.), Shock Compression of Condensed Matter, 1990, pp. 525–530.
[41]	S.T. Stewart, T.J. Ahrens, Shock wave propagation in porous ice, in: M.D. Furnish, L.C. Chhabildas, R.S. Hixson (Eds.), Shock Compression of Condensed Matter, American Institute of Physics, New York, 2000, pp. 1241–1244.
[42]	L.M. Barker, R.E. Hollenbach, Shock-wave studies of PMMA, fused silica and sapphire, J. Appl. Phys. 41 (10) (1970) 4208–4226.10.1063/1.1658439