PTFE/Al活性破片碰撞三层间隔靶冲击响应行为

Shock Response Behavior of PTFE/Al Reactive Fragment Impacting Three-Layer Spaced Target

  • 摘要: 为研究PTFE/Al活性破片多次碰撞下冲击响应行为,开展了活性破片碰撞三层间隔铝靶实验并采用包含自定义状态方程的数值方法进行模拟,定量分析了活性破片冲击激活反应行为的时空分布与毁伤效应. 结果表明,数值模拟中活性破片反应与空间分布情况与实验结果具有较好一致性,活性破片反应空间分布对中靶毁伤效果影响较大. 中靶厚3.0 mm时,各碰撞速度下活性破片均主要于中靶前方发生反应;中靶的穿孔面积与隆起范围随着碰撞速度增加而增大,且靶板隆起范围远大于穿孔面积. 中靶厚1.5 mm时,碰撞速度小于等于1100 m/s时活性破片主要于中靶后方发生反应,碰撞速度提升至1300 m/s后破片的主要反应位置转移至中靶前方;随着碰撞速度增加,中靶的穿孔面积呈先增大后减小趋势,隆起范围不断增加.

     

    Abstract: In order to study the shock response behavior of PTFE/Al fragments under multiple impacts, experiments of reactive fragments impacting three-layer spaced aluminum targets were carried out and the shock response behavior was simulated using a numerical method including custom state equation. The spatial and temporal distribution of impact ignition and reaction behavior and damage effect of reactive fragment were quantitatively analyzed. Results show that reaction and spatial distribution of reactive fragments in numerical simulation is in good agreement with experimental results. The temporal distribution of reactive fragment reaction has a great influence on the damage effect of the middle plate. When middle plate thickness is 3.0 mm, reaction of reactive fragments mainly occurs in front of the middle plate. Perforation area and uplift range of the target increase with the increase of impact velocity, and uplift range is much larger than perforation area. When middle plate thickness is 1.5 mm and impact velocity is less than or equal to 1 100 m/s, reaction of reactive fragments mainly occurs behind the middle plate. As impact velocity increases to 1 300 m/s, main reaction position of reactive fragments is transferred to the front of the middle plate. With the increase of impact velocity, perforation area of middle plate increases first and then decreases, and uplift range increases continuously.

     

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