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1. 北京理工大学 机电学院, 北京 100081
2. 湖南云箭集团有限公司, 湖南 长沙 410137
3. 北京理工大学 材料学院, 北京 100081
Received:19 June 2025,
Published Online:24 September 2025,
Published:30 September 2025
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Chenxu WANG, Jiahao ZHANG, Yiqiang CAI, et al. Explosion Driving Characteristics of Shell Fragments Driven by Cylindrical Charge with Cavity[J]. Acta Armamentarii, 2025, 46(9): 241089.
Chenxu WANG, Jiahao ZHANG, Yiqiang CAI, et al. Explosion Driving Characteristics of Shell Fragments Driven by Cylindrical Charge with Cavity[J]. Acta Armamentarii, 2025, 46(9): 241089. DOI: 10.12382/bgxb.2024.1089.
为研究带空穴柱形装药壳体破片爆炸驱动特性
揭示空穴装药结构对壳体破片初速的影响机理
利用数值仿真研究不同空穴锥角下壳体破片爆炸驱动过程和初速分布规律。通过分析稀疏波传播路径、速度损失系数和破片加速过程
拟合了壳体破片初速沿轴向分布函数
计算结果与数值仿真结果之间的相对误差不超过15%。研究结果表明:稀疏波的提前产生和横截面装填比的降低是破片初速下降的主要因素;非起爆端破片初速随空穴锥角的减小和空穴锥顶高度的增大而减小;非起爆端反射稀疏波为近似平面波且与空穴表面呈一定角度
稀疏波到达壳体的时间与壳体的轴向位置呈线性正相关关系;横截面装填比与
k
呈二次函数关系
k
为该横截面距非起爆端的长度和锥顶高度之间的比值
速度损失系数随比值
k
的减小呈指数形式衰减;研究成果可对破甲杀伤复合战斗部和带空穴结构的可变形破片战斗部的总体结构设计、材料选型及结构优化提供有益参考。
In order to study the explosion driving characteristics of shell fragments driven by cylindrical charge with cavity and reveal the mechanism of the influence of shaped charge structure on the initial velocity of shell fragments
the explosion driving process and initial velocity distribution of shell fragments under different cavity cone angles are studied through the numerical simulation.The initial velocity distribution function of shell fragment along the axial direction is fitted by analyzing the rarefaction wave propagation path
velocity loss coefficient and fragment acceleration process.The relative error between the calculated and simulated results is less than 15%.The results show that the earlier generation of rarefaction wave and the decrease in cross-section ratio of mass of c
harge to shell are the main factors contributing to the decrease in the initial velocity of fragments.The initial velocity of the fragments near the non-detonation end decreases with the decrease in the cone angle of cavity and the increase in the cone top height of cavity.The rarefaction wave reflected from the non-detonation end is an approximately planar wave and is at a certain angle to the cavity surface.The instant when rarefaction wave reaches shell is linearly and positively correlated with the axial position of the shell.The cross-section ratio of mass of charge to shell has a quadratic function relationship with
k
where
k
is the ratio of the distance from the cross section to the non-initiating end to the height of cavity cone top.The velocity loss coefficient decays exponentially with the decrease in
k
.The research can provide a useful reference for the overall structural design
material selection and structural optimization of anti-armour and anti-personnel composite warheads and the deformable fragment warhead with cavity charge structure.
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GAO Y G , FENG S S , LIU Y H , et al. Initial velocity distribution of fragments from cylindrical charge shells with different thick end caps [J ] . Acta Armamentarii , 2022 , 43 ( 7 ): 1527 - 1536 . (in Chinese) DOI: 10.12382/bgxb.2021.0443 http://doi.org/10.12382/bgxb.2021.0443 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.
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 , 2021 , 17 ( 3 ): 1052 - 1061 . DOI: 10.1016/j.dt.2020.06.024 http://doi.org/10.1016/j.dt.2020.06.024 The prediction of the fragment velocity distribution of a cylindrical cased charge with end caps is one of the key issues to assess the damage efficiency of the warhead. However, limited work has been conducted to predict the fragment velocity distributions along the axis of cylindrical cased charges with end caps. This paper presents a study of the velocity distribution of fragments caused by the explosion of a cylindrical cased charge with end caps. The fragment velocity distribution and the end cap velocity were determined by an X-ray radiography method, and the axial fragment distribution was determined by witness plates. It was found that the velocities of fragments, especially near the edge, were increased when the end caps were added, and the position of maximum velocity is closer to the non-detonation end. The fragment velocities were increased, and the fragment projection range was decreased with the increase of the thickness of the end cap. A formula for fragment velocity distributions of a cylindrical cased charge with end caps, which is based on Huang's formula, was proposed by the theoretical analysis and data fitting and validated experimentally. The results indicate that the proposed formula is accurate in predicting the fragment velocity distribution along the axis of a cylindrical cased charge with end caps detonated at one end. © 2020 The Authors
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