Hostname: page-component-78c5997874-m6dg7 Total loading time: 0 Render date: 2024-11-06T00:18:18.794Z Has data issue: false hasContentIssue false
  • English
  • Français

Dynamic compression of solid HMX-based explosives under ramp wave loading

Published online by Cambridge University Press:  05 November 2012

G.J. Wang ,
J.T. Cai ,
H.P. Zhang ,
F. Zhao ,
F.L. Tan  and
G. Wu
G.J. Wang*
Affiliation:
Institute of Fluid Physics, China Academy of Engineering Physics, 64 Mianshan road, Youxian block, Mianyang, Sichuan 621900, P.R. China
J.T. Cai
Affiliation:
Institute of Fluid Physics, China Academy of Engineering Physics, 64 Mianshan road, Youxian block, Mianyang, Sichuan 621900, P.R. China
H.P. Zhang
Affiliation:
Institute of Fluid Physics, China Academy of Engineering Physics, 64 Mianshan road, Youxian block, Mianyang, Sichuan 621900, P.R. China
F. Zhao
Affiliation:
Institute of Fluid Physics, China Academy of Engineering Physics, 64 Mianshan road, Youxian block, Mianyang, Sichuan 621900, P.R. China
F.L. Tan
Affiliation:
Institute of Fluid Physics, China Academy of Engineering Physics, 64 Mianshan road, Youxian block, Mianyang, Sichuan 621900, P.R. China
G. Wu
Affiliation:
Institute of Fluid Physics, China Academy of Engineering Physics, 64 Mianshan road, Youxian block, Mianyang, Sichuan 621900, P.R. China
*
ae-mail: [email protected]
Get access

Abstract

By means of the new techniques of magnetically driven quasi-isentropic compression based on compact capacitor bank facility CQ-1.5 developed by us, the dynamic compression of two mixed HMX-based plastic bonded explosives (PBX) explosives is researched under ramp wave loading. A pressure of 5–8 GPa over 600–800 ns is realized on explosive samples by optimizing loading electrodes and controlling charging voltages of CQ-1.5. And loading strain rates vary from 105 1/s to 106 1/s along the thickness of explosive samples. For experiments, the particle velocities of interface between explosive samples with different thicknesses and LiF windows are measured to determine material response by a displacement interferometry technique of Doppler pins system (DPS), and the experimental compression isentropes of researched explosives are obtained using the data processing method of backward integration and Lagrangian analysis for quasi-isentropic compression experiments, which are in agreement with the theoretical isentropes based on Mie-Grüneisen equation of state (EOS) and the results by Baer. For simulations, one-dimensional hydrodynamics code SSS is used to analyze the dynamic process, and the calculated results of particle velocity of interfaces are consistent with the experimental ones. Finally, one of the explosive constituents, the binder fluoride rubber F2311, is also investigated using this technique, and some properties under ramp wave loading are gained.

Type
Research Article
Information
The European Physical Journal - Applied Physics , Volume 60 , Issue 2: Topical issue: New trends in porous media. Edited by D. Salin , November 2012 , 21001
Copyright
© EDP Sciences, 2012

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Reisman, D.B. et al., in Isentropic Compression of LX-04 on the Z Accelerator, Shock Compression of Condensed Matter-2001, edited by Furnish, M.D., Thadhani, N.N., Horie, Y. (AIP Press, Atlanta, Georgia, USA, 2002), pp. 849–852Google Scholar
Hare, D.E. et al., in The Isentrope of Unreacted LX-04 to 170 kbar, Shock Compression of Condensed Matter-2003, edited by Furnish, M.D., Gupta, Y.M., Forbes, J.W. (AIP press, Portland, Oregon, USA, 2004), pp. 145–148Google Scholar
Quidot, M., Chabin, P., Constitutive model and equation of state of unreacted PBXN109, in 13th International Detonation Symposium, Norfolk, VA, USA, 2006Google Scholar
Ding, J.L., Asay, J.R., Int. J. Plast. 25, 695 (2009)CrossRef
Hall, C.A. et al., Rev. Sci. Instrum. 72, 3587 (2001)CrossRef
Baer, M.R. et al., Shockless Compression Studies of HMX-Based Explosives, in AIP Conf. Proc., Shock Compression of Condensed Matter (2009), Nashville, Tennessee, USA, 2010, pp. 699–702Google Scholar
Wang, G.J. et al., Rev. Sci. Instrum. 79, 53904 (2008)CrossRef
Aidun, J.B., Gupta, Y.M., J. Appl. Phys. 69, 60998 (1989)
Hayes, D., Technical Report SAND2001-1440, Sandia National Laboratories, 2001Google Scholar
Zhang, H.P. et al., Chin. J. Theor. Appl. Mech. 43, 105 (2011)
L’Eplattenier, P., Cook, G., Ashcraft, C., Introduction of an electromagnetism module in LS-DYNA for Coupled Mechanical Thermal Electromagnetic Simulations, in 3rd Int. Conf. on High Speed Forming, Dortmund, Germany, 2008Google Scholar
Baer, M.R., Hall, C.A., J. Appl. Phys. 101, 034906 (2007)CrossRef
Hare, D.E., Lawrence Livermore National Laboratory Report No. UCRL-TR-206486, 2004Google Scholar
Weng, J.D. et al., Rev. Sci. Instrum. 76, 093301 (2005)CrossRef
Dong, H.S., Performance of High Explosive and Correlates (Science Press, Beijing, 1989) [in Chinese]Google Scholar
Steinberg, D.J., Lawrence Livermore National Laboratory, UCRL-MA-106439, 1996Google Scholar
Sun, C.W., Chin. J. Comput. Phys. 3, 143 (1986)