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兵工学报 ›› 2022, Vol. 43 ›› Issue (9): 2399-2407.doi: 10.12382/bgxb.2022.0536

• 论文 • 上一篇    下一篇

超高速钢球打击肥皂与生物靶标的创伤弹道特点研究

李冠桦, 张良潮, 翁昌梅, 张东冬, 张洁元, 陈魁君, 段朝霞, 康建毅, 王建民   

  1. (陆军特色医学中心 武器杀伤生物效应评估研究室, 重庆 400042)
  • 上线日期:2022-08-21
  • 通讯作者: 王建民(1962—),男,研究员,博士生导师 E-mail:jmwang@mail.tmmu.edu.cn
  • 作者简介:李冠桦(1983—),男,实验师。E-mail: leeguanhua@qq.com
  • 基金资助:
    军队重大项目(ALJ18J001)

Study of Traumatic Ballistic Characteristics of Ultra-high Speed Steel Balls Striking Soap and Biological Targets

LI Guanghua, ZHANG Liangchao, WENG Changmei, ZHANG Dongdong, ZHANG Jieyuan,CHEN Kuijun, DUAN Chaoxia, KANG Jianyi, WANG Jianmin   

  1. (Department of Weapon Bioeffect Assessment, Army Specialty Medical Center, Chongqing 400042, China)
  • Online:2022-08-21

摘要: 通过对比研究不同速度钢球打击肥皂靶和生物靶的创伤弹道表现,探讨二者在超高速破片打击下的动态响应异同。采用不同速度(1 000 m/s、2 000 m/s、3 000 m/s、4 000 m/s)的0.72 g钢球分别打击肥皂靶和实验动物后肢肌肉丰满处。打击后观察靶标的弹道学表现,包括出入口大小、伤腔形状和大小、动物肢体损伤范围和损伤程度。研究结果表明:从1 000 m/s到4 000 m/s,随着钢球速度的增加,伤道入口越大,伤道出口从1 000 m/s到3 000 m/s逐渐增大;在4 000 m/s速度时,投射物未能穿出软组织,形成半球形伤腔;钢球以1 000 m/s速度打击肥皂时形成直径为5 cm的入口和直径0.6 cm大小的出口圆锥体;2 000 m/s速度打击肥皂时形成直径为16 cm的入口和出口直径3 cm大小的圆锥体;4 000 m/s速度打击肥皂时形成25 cm×25 cm×17 cm的半球形坑,未击穿肥皂;从弹道入口为起始点,以1 cm为间距分别测量的动物瞬时空腔、动物伤腔和肥皂空腔不同伤道深度上剖面投影的直径大小。对比相同速度钢球打击下剖面直径变化曲线,发现不同速度下伤道深度5~10 cm处肥皂空腔和动物的瞬时空腔的剖面直径相近。在超高速钢球打击下,肥皂靶形成的空腔与生物靶形成的瞬时空腔在伤道前端大小近似,可见肥皂靶可以一定程度上反映超高速钢球的生物杀伤效应。

关键词: 超高速钢球, 肥皂靶, 生物靶, 创伤弹道

Abstract: By comparing the traumatic ballistic performance of different velocities steel balls striking soap targets and biological targets, the similarities and differences of dynamic responses between the two under hypervelocity fragmentation strikes were explored. A 0.72 g steel ball with different velocities (1 000 m/s, 2 000 m/s, 3 000 m/s, 4 000 m/s) was used to strike the soap target and the hind limb muscle fullness of experimental animals, respectively. The ballistic manifestations of the targets were observed after the strikes, including the size of the entrance and exit, the shape and size of the wound cavity, the extent of injury and the degree of injury in the experimental animals. From 1 000 m/s to 4 000 m/s, the ballistic entrance became larger as the velocity of the steel ball increased. And the ballistic exit gradually increased from 1 000 m/s to 3 000 m/s. At 4 000 m/s velocity, the projectile failed to penetrate the soft tissue, forming a hemispherical wound cavity. The steel ball striking the soap at 1 000 m/s formed a 5 cm diameter entrance and 0.6 cm size exit cone; the steel ball striking the soap at 2 000 m/s formed a 16 cm diameter entrance and 3 cm size exit cone. 4 000 m/s speed striking the soap formed a 25 cm×25 cm×17 cm spherical crater, which did not penetrate the soap. The diameters of the profile projections on different wound depths of the animal transient cavity, animal wound cavity and soap cavity were measured from the ballistic entrance as the starting point at a spacing of 1 cm, respectively. Comparison of the profile diameter change curves under steel ball strikes at the same speed revealed that the profile diameters of the soap cavity and the animal transient cavity were similar at different wound depths of 5 cm to 10 cm at different speeds. Under the ultra-high speed steel ball strike, the cavity formed by the soap target and the transient cavity formed by the biological target at the front end of the wound channel were similar in size. The soap target can reflect the biocidal effect of the hypervelocity steel ball to some extent.

Key words: ultra-highspeedsteelball, soaptarget, biologicaltarget, traumaticballistic

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