Laser driven explosion and shock wave: a review
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摘要: 随着高功率密度激光技术的快速发展，强激光驱动的爆炸与冲击效应逐渐引起国内外学者的广泛关注。对强激光诱导爆炸与冲击效应研究进展进行了综述，包括强激光诱导爆炸载荷特征与相似律，强激光对材料表面冲击强化处理，强激光冲击诱导材料相变动力学行为，以及利用强激光驱动微弹道冲击等方面的研究进展，并指出了强激光诱导爆炸与冲击效应研究的发展趋势和未来需要解决的关键科学问题。Abstract: With the rapid development of high-power density laser, the laser driven explosion and shock waves have attracted great attention in recent years. In this paper, the progress of laser driven explosion and shock waves, involving the laser explosive loading characteristics and the scaling law, the laser shock peening of material, the dynamic phase-transformation behavior of materials under laser shock, and the laser-induced micro-bullet impact, is reviewed.
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图 3 (a)强激光驱动爆炸与冲击效应相似律分析方法；(b)约束层厚度对强激光冲击的饱和效应；(c)激光脉宽和(d)激光能量对表面残余压应力幅值与塑性区深度的影响规律[27]
Figure 3. (a) Parameters of laser, confined overlayer, metallic target. (b) Influence of thickness in confined overlayer on shock effect. (c) Influence of laser duration on shock effect. (d) Influence of laser power density on shock effect[27]
图 7 激光水下烧蚀非晶合金的在位观察结果。捕捉到高温物质的喷发，并伴随着空化气泡的扩张。底部时间轴表示烧蚀中各个物理过程的时间关系[62]
Figure 7. Ejection of the high-temperature matter with an evolving bubble after single-shot nanosecond pulse laser ablation of the metallic glass target in water. The sketch at the bottom of the figure shows the main stages during the pulse laser ablation[62]
图 15 (a) 冲击速度与CNT薄膜比吸能的关系；(b) 纳米厚度的CNT薄膜的比吸能与其他材料的对比[95]；(c) 比吸能随交联密度的变化[94]；(d) 不同交联密度CNT薄膜的ΔEs/ΔEb变化历程[94]；(e) 未添加交联和交联密度为20时CNT薄膜的穿孔形貌变化[94]
Figure 15. (a) Relationship between impact velocity and SEA of CNT film. (b) Comparison of SEA[95].(c) Relationship between SEA and crosslink density[94]. (d) Evolution of ΔEs/ΔEb of CNT film with different crosslink density[94]. (e) Penetration morphologies change of CNT film before and after adding crosslinks[94]
图 17 (a) PS薄膜比吸能与缠结度之间的关系[98]；(b) PS薄膜与PC薄膜的失效形貌对比；(c) 沿不同方向冲击时块层状纳米复合材料的微观结构变化[100]；(d) P(VDF-TrEE)薄膜的比吸能[101]
Figure 17. (a) Relationship between SEA of PS film and entanglement degree [98]. (b) Failure morphologies of PS film and PC film. (c) Micro-structure change of bulk lamellar nanocomposite under impact along different directions[100]. (d) SEA value of P(VDF-TrEE) thin film[101]
图 18 (a)微颗粒碰撞铝金属靶板时的反弹与粘合过程；其中上下两行的多帧序列分别显示了铝颗粒在阈值速度以下（605 m/s）和以上（805 m/s）对铝靶板的影响[102]； (b)金属材料的动态硬度计算结果[104]。(c) 熔化驱动的不同颗粒/基体材料组合触发熔体驱动侵蚀的冲击速度图谱[105]
Figure 18. (a) In-situ observation of the re-bounding and bonding moment in microparticle impact. Multi-frame sequences at top and bottom showing the Al particle impacts on Al substrate below (605 m/s) and above (805 m/s) the critical velocity[102]. (b) Calculation results of dynamic hardness of metallic materials[104]. (c) Melt-driven erosion map. Impact velocity at which melt-driven erosion is triggered for different combinations of particle/substrate materials[105]
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