WANG Jin,LIU Yize,ZHANG Hongyu, YAN Yueguang,WANG Haifu,GE Chao
Acta Armamentarii. 2024, 45(S1):
161-173.
Linear focusing fragment warhead makes the fragments disperse at an equal velocity and focus linearly by taking advantage of the design of charge generatrix and fragment arrangement, which can exert structural cutting damage to a target. In order to study the influence of structural parameters of linear focusing fragment warhead on the dispersion characteristics of fragments, the fluid-structure interaction (FSI) algorithm is used to numerically simulated the focusing process of fragments. The numerically simulated results reveal the linear focusing mechanism of linear focusing fragment warhead. The typical linear focusing process includes fragment driving stage, fragment focusing stage, focusing completion stage and fragment dispersion stage. The effects of warhead size, fragment arrangement, fragment mass and intersection velocity on the dispersion and spatial distribution characteristics of fragments are further obtained by numerical simulation. The results show that, with the increase in charge length from 0.3 m to 0.5 m, the standard deviation of fragment velocity increases from 125 m/s to 147 m/s, the focusing completion time is 490 μs, 585 μs and 590 μs, respectively, and the width of perforation dense distribution increases from 135 mm to 234 mm. When the fragment arrangement increases from 15 columnsto 18 columns, the standard deviation of fragment velocity increases from 117 m/s to 125 m/s, the focusing completion time is 470 μs and 490 μs, respectively, and the width of perforation dense distribution increases from 235 mm and 135 mm respectively. When the fragment mass increases from 4.08 g to 9.21 g, the standard deviation of fragment velocity decreases from 137 m/s to 125 m/s, the focusing completion time is 380 μs and 490 μs, and the width of perforation dense distribution is 156 mm and 135 mm, respectively. When the interaction speed increases from 0 m/s to 1 000 m/s, the focusing completion time is 490 μs, 480 μs and 469 μs, respectively, the width of perforation dense distribution increases from 135 mm to 138 mm, and the density of fragment distribution decreases from 640/m2 to 630/m2with a rate of about 2%. The research results can provide guidance and reference for the design of focusing warhead.