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

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

doi:10.1016/j.mre.2017.02.001

[1] V.M. Zaitzev, P.F. Pokhil, K.K. Shvedov, the Electromagnetic Method for We thank Professor Yihong Hang, Professor Heng Yu, and Professor Xin Yu worked at Institute of Applied Physics and Computation Mathematics for their support in this project. The development of the experiments was funded by China Acad-emy of Engineering Physics. e 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 SurfaceWeapons 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.

[6] R. Fowles, R.F. Williams, Plane wave stress propagation in solids, J. Appl. Phys. 41 (1) (1970) 360-365.

[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.

[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.

[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] 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.

[20] E. Barsis, E. Williams, C. Skoog, Piezoresistivity coefficients in manganin, J. Appl. Phys 41 (1980) 5155-5162.

[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.

[22] Z. Rosenberg, Y. Partom, Lateral stress measurement in shock-loaded targets with transverse piezoresistive gauges, J. Appl. Phys. 58 (1985) 3072-3076.

[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.

[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. (Eds.), 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.

[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.

[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 shockinduced 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 studiesdsugar 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, Stressestrain response of PBX 9501 below 1 gigapascal from embeddedmagnetic 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 buildup 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.

[39] 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.

[40] 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.

[41] L.M. Barker, R.E. Hollenbach, Shock-wave studies of PMMA, fused silica and sapphire, J. Appl. Phys. 41 (10) (1970) 4208-4226.