爆炸冲击下氟壳铝释能特性试验研究

Experimental Study on the Energy Release Characteristics of Fluorine Shell Aluminum Under Blast Impact

  • 摘要: 为研究爆炸冲击下该材料的点火释能特性,开展该材料点火释能特性相关试验研究. 首先,基于TG-DSC试验,空气中缓慢加热氟壳铝,分析得到其主要放热过程为氟聚合物外壳破碎后活性纳米铝粉与空气中氧气反应阶段,通过激光点火试验结果与文献分析得到了常温常压下氟壳铝点火延时为Al/PTFE材料的60.49%,燃速为Al/PTFE的289.71%;然后,压制了Al/PTFE和氟壳铝两种活性材料药块,分别开展雷管、JHL-2炸药对两种材料的爆炸冲击点火试验. 试验发现:雷管爆炸冲击下氟壳铝自持反应能力比Al/PTFE更好,氟壳铝反应速率为Al/PTFE的1.38倍;JHL-2炸药爆炸冲击下氟壳铝和Al/PTFE均增加了火球面积,增加量分别为28.17%、31.62%;同时得到爆炸火球面积最大值达到时间氟壳铝较Al/PTFE快31.21%;JHL-2引爆氟壳铝相比雷管引爆JHL-2在距爆心2 、3 、4 m处自由场超压比冲量皆有提升,最大提升量124.6%,自由场超压比冲量随冲击波传播距离下降速度变缓,衰减速率最大降低12.18%. 最后,总结爆炸冲击下氟壳铝整体反应分为3个阶段:炸药爆炸初始阶段氟壳铝部分反应—未反应氟壳铝破碎成颗粒飞散—氟壳铝颗粒脱离爆炸真空域与空气接触点火爆燃完全,氟壳铝释能过程集中在第3阶段. 氟壳铝在爆炸冲击下的增能效果主要体现在提升爆炸热毁伤能力与提升爆炸冲击波比冲量并延缓冲击波衰减.

     

    Abstract: To study the ignition and energy release characteristics of this material under explosive shock, relevant experiments were conducted. First, based on TG-DSC experiments, the Fluorine Shell Aluminum was slowly heated in air, revealing that the main exothermic process occurs when the fluoropolymer shell breaks down and the active nano-aluminum reacts with oxygen in the air. Laser ignition test results and literature analysis showed that at normal temperature and pressure, the ignition delay of Fluorine Shell Aluminum is 60.49% of that of Al/PTFE, and its burning rate is 289.71% of Al/PTFE. Then, Al/PTFE and Fluorine Shell Aluminum were pressed into reactive material pellets, and explosive shock ignition tests were conducted using a detonator and JHL-2 explosives on both materials. The tests reveal that under detonator-induced shock, Fluorine Shell Aluminum had a better self-sustaining reaction capability than Al/PTFE, with a reaction rate 1.38 times that of Al/PTFE. Under explosive shock, both Fluorine Shell Aluminum and Al/PTFE increased the fireball area by 28.17% and 31.62%, respectively. The time to reach the maximum fireball area for Fluorine Shell Aluminum was 31.21% faster than for Al/PTFE. Additionally, when JHL-2 initiated Fluorine Shell Aluminum compared to detonator-initiated JHL-2, the free-field overpressure impulse at 2 m, 3 m, and 4 m from the explosion center increased, with the maximum increase being 124.6%. The rate of decline in free-field overpressure impulse slowed with the propagation distance of the shockwave, with the maximum attenuation rate reduced by 12.18%. Finally, the overall reaction process of Fluorine Shell Aluminum under explosive shock was summarized in three stages: a partial reaction occurs during the initial detonation phase; the unreacted Fluorine Shell Aluminum fragments into dispersed particles; and these particles exit the explosion’s vacuum zone, come into contact with air, ignite, and proceed to complete deflagration. The energy release from Fluorine Shell Aluminum is predominantly concentrated in the third stage. The energy-enhancing effects of Fluorine Shell Aluminum under explosive shock are mainly reflected in the increased thermal damage capability of the explosion and the enhanced shockwave impulse, as well as the delayed attenuation of the shockwave.

     

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