Initial Velocity Distribution of Fragments from Cylindrical Charge Shells with Different Thick End Caps

GAO Yueguang;FENG Shunshan;LIU Yunhui;HUANG Qi

Acta Armamentarii ›› 2022, Vol. 43 ›› Issue (7) : 1527-1536. DOI: 10.12382/bgxb.2021.0443
Paper

Initial Velocity Distribution of Fragments from Cylindrical Charge Shells with Different Thick End Caps

  • GAO Yueguang, FENG Shunshan, LIU Yunhui, HUANG Qi
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Abstract

The end cap thickness is an important factor to be considered in the accurate design of fragmentation warheads, so this study focues on the initial velocity distribution of fragments from cylindrical charge shell with different thick end caps, which is detonated at the center of one end. Based on theoretical analysis and SPH numerical simulation, the models of cylindrical shells are established, and then the theoretical formula of axial distribution of the initial fragment velocity is proposed. The results show that, with the increase in thicknesses of two end caps, the effect of axial rarefaction waves decreases, and the fragment velocity near the two ends increases accordingly. The acceleration effect of detonation products is the main cause of the velocity increase of fragments near the detonation end, while the acceleration effect of detonation waves is the main cause of the velocity increase of fragments near the non-detonation end. Compared with the fragments near the detonation end, the acceleration of the fragments near the non-detonation end is more apparent. The proposed formula is more suitable for end caps and materials in engineering and the relative error can be significantly reduced. The findings of this study can provide reference for the accurate design of warheads.

Key words

ordnancescienceandtechnology / initialfragmentvelocity / Gurneyequation / axialrarefactionwaves / numericalsimulation

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GAO Yueguang, FENG Shunshan, LIU Yunhui, HUANG Qi. Initial Velocity Distribution of Fragments from Cylindrical Charge Shells with Different Thick End Caps. Acta Armamentarii. 2022, 43(7): 1527-1536 https://doi.org/10.12382/bgxb.2021.0443

References


[1]STRONGEW J, MA X, ZHAO L. Fragmentation of explosively expanded steel cylinders[J]. International Journal of Mechanical Sciences, 1989, 31(11/12): 811-823.
[2]李铁鹏. 战斗部破片初速分布及空间数量分布[D]. 南京:华东工学院, 1988.
LI T P. The distribution of warhead fragment muzzle velocity and space quantity[D]. Nanjing:East China Industrial Engineering Institute, 1988. (in Chinese)
[3]王志军, 尹建平. 弹药学[M]. 北京:北京理工大学出版社, 2005.
WANG Z J, YIN J P. Ammunition[M]. Beijing: Beijing Institute of Technology Press, 2005. (in Chinese)
[4]GURNEY R W. The initial velocities of fragments from bombs, shell, grenades[R]. BRL Report 405, 1943.
[5]BOLAM S, MADAN A K, SINGH M, et al. Expansion of metallic cylinders under explosive loading[J]. Defence Science Journal, 2013, 42(3): 157-163.
[6]GAO Y G, FENG S S, ZHANG B, et al. Effect of the length-diameter ratio on the initial fragment velocity of cylindrical casing[J]. IOP Conference Series Materials Science and Engineering, 2019, 629(1): 012-020.
[7]冯顺山, 崔秉贵. 战斗部破片初速轴向分布规律的实验研究[J]. 兵工学报, 1987, 11(4): 60-63.
FENG S S, CUI B G. An experimental investigation for the axial distribution of initial velocity of shells[J]. Acta Armamentarii, 1987, 11(4): 60-63. (in Chinese)
[8]印立魁, 蒋建伟, 门建兵,等. 立方体预制破片战斗部破片初速计算模型[J]. 兵工学报, 2014, 35(12): 1967-1971.
YIN L K, JIANG J W, MEN J B, et al. An initial velocity model of explosively-driven cubical fragments[J]. Acta Armamentarii, 2014, 35(12): 1967-1971. (in Chinese)
[9]HUANG G Y, LI W, FENG S S. Axial distribution of Fragment Velocities from cylindrical casing under explosive loading[J]. International Journal of Impact Engineering, 2015, 76: 20-27.
[10]KONGX, WU W, LI J, et al. A numerical investigation on explosive fragmentation of metal casing using Smoothed Particle Hydrodynamic method [J]. Materials and Design, 2013, 51(60):729-741.
[11]GUOZ W, HUANG G Y, ZHU W, et al. Mechanism and suppression of the effect of axial rarefaction waves on the eccentric initiation effect [J]. International Journal of Impact Engineering, 2018, 124: 37-47.
[12]GAO Y G, FENG S S, YAN X M, et al. Axial distribution of fragment velocities from cylindrical casing with air parts at two ends [J]. International Journal of Impact Engineering, 2020, 140: 44-57.
[13]RANDLESP W, LIBERSKY L D. Smoothed particle hydrodynamics: some recent improvements and applications[J]. Computer Methods in Applied Mechanics & Engineering, 1996, 139(1-4): 375-408.
[14]RABCZUKT, EIBL J. Modelling dynamic failure of concrete with meshfree methods[J]. International Journal of Impact Engineering, 2006, 32(11): 1878-1897.
[15]HAYHURSTC J, CLEGG R A. Cylindrically symmetric SPH simulations of hypervelocity impacts on thin plates[J]. International Journal of Impact Engineering, 1997, 20(1-5): 337-348.
[16]张雁思, 戴文喜, 王志军. 基于SPH算法的爆破战斗部壳体破碎数值仿真研究[J]. 兵器材料科学与工程, 2015,38(5): 85-88.
ZHANG Y S, DAI W X, WANG Z J. Numerical simulation of blasting warheads shell breaking based on SPH method[J]. Ordnance Material Science and Engineering, 2015, 38(5): 85-88.(in Chinese)
[17]LIW, HUANG G Y, FENG S S. Effect of eccentric edge initiation on the fragment velocity distribution of a cylindrical casing filled with charge[J]. International Journal of Impact Engineering, 2015, 80: 107-115.
[18]陈刚,陈忠富,陶俊林,等.45钢动态塑性本构参量与验证[J]. 爆炸与冲击, 2005, 25(5): 69-74.
CHEN G, CHEN Z F, TAO J L, et al. Investigation and validation on plastic constitutive parameters of 45 steel [J]. Explosion and Shock Waves, 2005,25(5): 69-74. (in Chinese)
[19]DYNAMICSC. Release 14.0 documentation for ANSYS AUTODYN[Z]. US: ANSYS Inc., 2011: 150-151.
[20]LIAO W, JIANG J W, MEN J B, et al. Effect of the end cap on the fragment velocity distribution of a cylindrical cased charge[J]. Defence Technology, 2020, 17(3): 1052-1061.
[21]PREDEBONW W, SMOTHERS W G, ANDERSON C E. Missile warhead modeling: computations and experiments[R]. 1977, ADA047294.

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