Elastic-plastic transition behaviors of HMX crystal under ramp wave compression

CHONG Tao; MO Jianjun; ZHENG Xianxu; FU Hua; CAI Jintao

doi:10.11883/bzycj-2020-0071

Volume 41 Issue 5

May 2021

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CHONG Tao, MO Jianjun, ZHENG Xianxu, FU Hua, CAI Jintao. Elastic-plastic transition behaviors of HMX crystal under ramp wave compression[J]. Explosion And Shock Waves, 2021, 41(5): 053101. doi: 10.11883/bzycj-2020-0071

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CHONG Tao, MO Jianjun, ZHENG Xianxu, FU Hua, CAI Jintao. Elastic-plastic transition behaviors of HMX crystal under ramp wave compression[J]. Explosion And Shock Waves, 2021, 41(5): 053101. doi: 10.11883/bzycj-2020-0071

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Elastic-plastic transition behaviors of HMX crystal under ramp wave compression

doi: 10.11883/bzycj-2020-0071

Institute of Fluid Physics, China Academy of Engineering Physics, Mianyang 621999, Sichuan, China

Received Date: 2020-03-19
Rev Recd Date: 2020-12-04

Available Online: 2021-03-18

Publish Date: 2021-05-05

Abstract

Abstract

The dynamics of HMX single crystals under ramp wave loading was studied experimentally and numerically. The ramp wave compression experiments of (010) and (011) crystal oriented HMX crystals within 15 GPa were carried out with the magnetic driven device CQ-4, which can provide a loading pressure with a rising time of 450−600 ns. The velocity curves of the interface between the HMX single crystal and the LiF single crystal were obtained with dual laser heterodyne velocimetry (DLHV). The experimental results show that there is an obvious elastic-plastic transition behavior in the loading section. The velocity waveforms have a downward trend in the elastic-plastic transition section, which is caused by the viscous effect of the HMX single crystal. The elastic limit of the HMX single crystal changes with the increase of the sample thickness. The Lagrange sound speed-particle velocity data and pressure-specific volume curves of (010) and (011) crystal oriented HMX crystals were obtained with the iterative Lagrange data processing method for dynamic impedance mismatch. The Lagrange sound speed-particle velocity relationships in the different crystal directions are different. The pressure-specific volume curve is close to isentropic experimental data by Sandia laboratory. The numerical simulation of the physical process of ramp wave compression of the HMX crystal was carried out with the viscoelastic plastic constitutive relation of Hobnemser-Prager and the third-order Birch-Murnaghan equation of state. The calculation results can well describe the physical process of the elastic-plastic transformation of HMX crystal.
- HMX crystal,
- elastic-plastic transition,
- ramp wave compression,
- equation of state

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References(32)

References

[1]	谭武军. 含能晶体力学性能研究[D]. 绵阳: 中国工程物理研究院, 2008. TAN W J. Studies on the mechanical properties of energetic crystals [D]. Mianyang: China Academy of Engineering Physics, 2008.
[2]	李明, 陈天娜, 黄明, 等. RDX晶体的破碎与细观断裂行为 [J]. 含能材料, 2013, 21(2): 200–204. DOI: 10.3969/j.issn.1006-9941.2013.02.008. LI M, CHEN T N, HUANG M, et al. Rupture and mesoscale fracture behaviors of RDX crystals [J]. Chinese Journal of Energetic Materials, 2013, 21(2): 200–204. DOI: 10.3969/j.issn.1006-9941.2013.02.008.
[3]	王国栋, 刘玉存. 神经网络在炸药晶体密度预测中的应用 [J]. 火炸药学报, 2007, 30(1): 57 –59. DOI: 10.3969/j.issn.1007-7812.2007.01.016. WANG G D, LIU Y C. Application of artificial neural network in predicting the density of explosives [J]. Chinese Journal of Explosives and Propellants, 2007, 30(1): 57 –59. DOI: 10.3969/j.issn.1007-7812.2007.01.016.
[4]	花成, 傅华, 田勇, 等. 冲击波作用下HMX晶体的细观响应 [J]. 火炸药学报, 2010, 33(3): 5– 8. DOI: 10.3969/j.issn.1007-7812.2010.03.002. HUA C, FU H, TIAN Y, et al. Mesoscale response of HMX crystal under the shock war effect [J]. Chinese Journal of Explosives and Propellants, 2010, 33(3): 5– 8. DOI: 10.3969/j.issn.1007-7812.2010.03.002.
[5]	黄明, 李洪珍, 徐容, 等. 高品质 RDX 的晶体特性及冲击波起爆特性 [J]. 含能材料, 2011, 19(6): 621–626. HUANG M, LI H Z, XU R, et al. Evaluation of crystal properties and initiation characteristics of decreased sensitivity RDX [J]. Chinese Journal of Energetic Materials, 2011, 19(6): 621–626.
[6]	HOWE P M. Effects of microstructure on explosive behavior [J]. Progress in Astronomics and Aeronautics, 2000, 185: 141.
[7]	JOHANSEN Ø H, KRISTIANSEN J D, GJERSØE R, et al. RDX and HMX with reduced sensitivity towards shock initiation-RS-RDX and RS-HMX [J]. Propellants, Explosives, Pyrotechnics, 2008, 33(1): 20–24. DOI: 10.1002/prep.200800203.
[8]	VAN DER HEIJDEN A E D M, BOUMA R H B, VAN DER STEEN A C. Physicochemical parameters of nitramines influencing shock sensitivity [J]. Propell. Explos. Pyrotech, 2004, 29(5): 304–313. DOI: 10.1002/prep.200400058.
[9]	WALLEY S M, FIELD J E, GREENAWAY M W. Crystal sensitivities of energetic materials [J]. Materials Science and Technology, 2006, 22(4): 402–413. DOI: 10.1179/174328406X91122.
[10]	CAULDER S M, MILLER P J, GIBSON K D, et al. Effect of particle size and crystal quality on the critical shock initiation pressure of RDX/HTPB formulations [C]// Proceedings of 13th Symposium (International) on Detonation. Norfolk, VA, USA, 2006: 656–661.
[11]	VANDER STEEN A C, VERBEEK H, MEULENBRUGGE J J. Influence of RDX crystal shape on the shock sensitivity of PBXs [C]// Proceedings of 9th Symposium (International) on Detonation. Portland, Oregon, USA, 1989: 83–88.
[12]	花成, 张盛国, 高大元. 冲击波作用下炸药安全性QMU评估 [J]. 火炸药学报, 2015, 38(4): 31–34. HUA C, ZHANG S G, GAO D Y. QMU evaluation of explosive safety under shock wave effect [J]. Chinese Journal of Explosives and Propellants, 2015, 38(4): 31–34.
[13]	GOETZ F, BRILL T B, FERRARO J R. Pressure dependence of the raman and infrared spectra of α-, β-, γ-, and δ-octahydro-1, 3, 5, 7-tetranitro-1, 3, 5, 7-tetrazocine [J]. Journal of Physics Chemistry B, 1978, 82(17): 1912–1917. DOI: 10.1021/j100506a011.
[14]	CHOI C S, BOUTIN H P. A study of the crystal structure of β-cyclotetramethylene tetranitramine by neutron diffraction [J]. Acta Crystallographica Section B, 1970, 26(9): 1235–1240. DOI: 10.1107/S0567740870003941.
[15]	HORST J H, KRAMER H J M, ROSMALEN G M, et al. Molecular modelling of the crystallization of polymorphs: Part Ⅰ: the morphology of HMX polymorphs [J]. Journal of Crystal growth, 2002, 237: 2215–2220.
[16]	CLEMENTS B E, MAS E M. A theory for plastic-bonded materials with a bimodal size distribution of filler particles [J]. Modelling and Simulation in Materials Science and Engineering, 2004, 12(3): 407–421. DOI: 10.1088/0965-0393/12/3/004.
[17]	MENIKOFF R, DICK J J, HOOKS D E. Analysis wave profiles for single-crystal cyclotetramethylene tetranitramine [J]. Journal of Applied Physics, 2005, 97(2): 023529. DOI: 10.1063/1.1828602.
[18]	DICK J J, HOOKS D E, MENIKOFF R, et al. Elastic-plastic wave profiles in cyclotetramethylene tetranitramine crystals [J]. Journal of Applied Physics, 2004, 96(1): 374–379.
[19]	JARAMILLO E, SEWELL T D. Inelastic Deformation in shock loaded: HMX LA-UA-06-3716 [R]. Los Alamos National Laboratory Report, 2005.
[20]	SEWELL T D, BEDROV D, MENIKOFF R, et al. Elastic properties of HMX [J]. AIP Conference Proceedings, 2002, 620(1). DOI: 10.1063/1.1483562.
[21]	ZAUG J M. Elastic constants of β-HMX and tantalum, equation of state of supercritical fluids and fluid mixtures and thermal transport determinations [C]//The 11th International Detonation Symposium. Snowmass Conference Center. Snowmass Village, Colorado. 1998: 498−509.
[22]	HALL C A, ASAY J R, KNUDSON M D, et al. Experimental configuration for isentropic compression of solids using pulsed magnetic loading [J]. Review of Scientific Instruments, 2001, 72(9): 3587–3595. DOI: 10.1063/1.1394178.
[23]	YOO C S, CYNN H. Equation of state, phase transition, decomposition of β-HMX (octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine) at high pressures [J]. The Journal of Chemical Physics, 1999, 111(22): 10229. DOI: 10.1063/1.480341.
[24]	OLINGER B, ROOF B and CADY H H. The linear and volume compression of β-HMX and RDX [C]//Actes du Symposium International sur le Comportement des Milieux Denses Sous Hautes Pressions Dynamiques, Commissariat a l’Energie Atomique, Paris, 1978: 3−8.
[25]	MARSH S. LASL shock Hugoniot data [M]. Berkeley: University of California Press, 1980.
[26]	DANIEL, HOOK E and HAYES D B. Isentropic compression of cyclotetramethylene tetranitramine (HMX) single crystals to 50 GPa [J]. The Journal of Applied Physics, 2006, 99(12): 124901. DOI: 10.1063/1.2203411.
[27]	苏锐, 龙瑶, 姜胜利, 等. 外部压力下β相奥克托金晶体弹性性质变化的第一性原理研究 [J]. 物理学报, 2012, 16(20): 336–341. SU R, LONG Y, JIANG S L, et al. Elastic properties of β–HMX under extra pressure: a first principle study [J]. Acta Physica Sinica, 2012, 16(20): 336–341.
[28]	罗斌强, 张红平, 种涛, 等. 磁驱动斜波压缩实验结果的不确定度分析 [J]. 高压物理学报, 2017, 31(3): 295–300. DOI: 10.11858/gywlxb.2017.03.011. LUO B Q, ZHANG H P, CHONG T, et al. Experimental uncertainty analysis of magnetically driven ramp wave compression [J]. Chinese Journal of High Pressure Physics, 2017, 31(3): 295–300. DOI: 10.11858/gywlxb.2017.03.011.
[29]	BAER M, ROOT S, DATTELBAUM D, et al. Shockless compression studies of HMX-based and TATB-based explosives [C] // The 16th APS Topical Conference on Shock Compression of Condensed Matter. Nashville, Tennessee, 2009:699–702.
[30]	贾乃文. 粘塑性力学及工程应用 [M]. 北京: 地震出版社, 2000.
[31]	HRBEK G M. Invariant functional forms for the second, third, and fourth order Birch-Murnaghan equation of state for materials subject to hydrodynamic shock. [J]. Aip Conference Proceedings, 2000, 505(1): 169–173. DOI: 10.1063/1.1303448.
[32]	郭昕, 南海, 齐晓飞, 等. RDX和HMX晶体力学性能的分子动力学模拟及其撞击加载响应 [J]. 含能材料, 2013, 21(4): 485–489. DOI: 10.3969/j.issn.1006-9941.2013.04.016. GUO X, NAN H, QI X F, et al. Molecular dynamics simulation on mechanical properties of RDX and HMX crystals and their impacting loading response [J]. Chinese Journal of Energetic Materials, 2013, 21(4): 485–489. DOI: 10.3969/j.issn.1006-9941.2013.04.016.