摘要
针对低附带弹药毁伤需求,设计了一种十字形内置破片定向战斗部,根据目标方位可选择不同起爆模式,进而控制破片的径向飞散特性,在目标区域内形成杀伤破片实现定向毁伤,在非目标区域内实现低附带毁伤。采用数值模拟研究了相邻2点起爆、相邻3点起爆两种模式下定向战斗部起爆时破片的驱动过程,给出了各个位置处破片的飞散速度、径向飞散角度等特征参数;制备了2发单元样弹并开展了地面静爆实验,通过高速摄影及靶板上破片的穿孔分布特征实测出破片的速度及径向飞散角,与数值模拟结果对比,验证了模拟的准确性。在此基础上,通过引入能量分配角建立了破片速度的修正公式,并根据模拟结果对公式参数进行了拟合分析。结果表明:相邻2点起爆、相邻3点起爆模式下,战斗部定向杀伤区破片径向飞散角分别控制在145°、65°以内,且该区域内的破片占破片总数的比例分别达到了50.4%、43%;同时,破片速度呈现梯次分布,介于535~770 m/s之间,对1.5 mm厚的Q235A钢板的穿甲率分别达到了94.4%、84.6%,可实现对轻型车辆类目标的毁伤,其余区域则为低附带安全区;基于能量分配模型求得的破片速度理论计算值与模拟值基本吻合。研究结果可为低附带杀伤战斗部研制提供新的设计思路。
In order to meet the demand of low collateral damage,a cross-shape built-in fragmentation directional warhead was invented,which can select different detonation modes according to the target orientation and then control the radial dispersion characteristics of the fragmentation,in which the formation of anti-personnel fragmentation in the target area to achieve directional damage,while in the non-target area to achieve low collateral damage.Numerical simulation was used to study the fragmentation driving process during the detonation of the directional warhead in two modes:adjacent two-point detonation and adjacent three-point detonation.The characteristic parameters such as fragment dispersion velocity and radial dispersion angle were given at each position.Then,two principle samples were prepared and ground static explosion tests were conducted.The fragment velocity and radial dispersion angle were measured through high-speed photography and the distribution characteristics of fragment perforation on the target plate.The accuracy of the simulation is verified by comparing with the numerical simulation results,based on which the fragmentation velocity correction formula is established by introducing the energy distribution angle,and the parameters of the formula are fitted and analyzed according to the simulation results.The results show that the radial dispersion angle of fragments in the directed killing zone is controlled within 145°and 65°under adjacent two-point initiation and adjacent three-point initiation modes respectively,and the proportion of fragments in this area reaches 50.4%and 43%of the total number,respectively.The fragment velocity shows a graded distribution between 535 and 770 m/s.The penetration rate of 1.5 mm thick Q235A steel plate reaches 94.4%and 84.6%respectively,which can achieve the destruction of light vehicle type targets,while the rest of the area is a low incidental safety zone.The calculation result of fragment velocity based on the energy distribution model is basically consis
作者
李鑫
王伟力
梁争峰
畅波
苗润源
LI Xin;WANG Weili;LIANG Zhengfeng;CHANG Bo;MIAO Runyuan(College of Ordnance Engineering,Naval University of Engineering,Wuhan 430033,Hubei,China;Xi’an Modern Chemistry Research Institute,Xi’an 710065,Shaanxi,China)
出处
《爆炸与冲击》
EI
CAS
CSCD
北大核心
2023年第8期54-64,共11页
Explosion and Shock Waves
关键词
十字形
定向战斗部
低附带毁伤
破片速度
径向飞散角
能量分配模型
cross-shape
directional warhead
low collateral damage
fragment velocity
radial dispersion angle
energy distribution model
