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Characteristics of Plasma and Detonation Waves Induced on an Aluminum Target by Nanosecond Laser Ablation

机译:纳秒激光烧蚀对铝靶材产生的等离子体和爆轰波的特性

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摘要

Investigation of plasma and detonation wave characteristics induced by laser ablating target is very important to recognizing the mechanism of laser driven flyer and laser destruction. In this study a laser ablating aluminium target experiment has been carried out, employing Schlieren photography technique for visualizing detonation wave temporal evolution and to analyse detonation wave attenuation law. A numerical model of detonation wave evolution induced by laser ablation has been established: phase transformation volume fraction is employed to describe target vaporization; plasma state equation is obtained by calculating vapour ionization degree; interaction of laser and plasma is considered. Numerical simulation of laser ablating aluminium target has been conducted, analysing the unsteady ablation process of target. Comparison of shockwave propagation speed and compressed air thickness between calculated results and experimental data validates the calculation method. Results show that shockwave evolution has a complicated structure with multi-density discontinuities. During detonation wave evolution, wave front transforms from half elliptical in early stage into half spherical and peak density location changes from wave front to interior. The fluctuating range of target ablation rate under laser action (672 mJ, duration is 24 ns) is 0.08 to 0.32 mms. Plasma density distribution is related to laser energy variation. After laser pulse, ionization degree and electron number density of plasma first decreases slowly and then dropped dramatically.
机译:研究激光烧蚀靶引起的等离子体和爆轰波特性对于认识激光驱动飞片和激光破坏的机理非常重要。在这项研究中,已经进行了激光烧蚀铝靶的实验,采用Schlieren摄影技术可视化了爆炸波的时间演化并分析了爆炸波的衰减规律。建立了由激光烧蚀引起的爆轰波演化的数值模型。通过计算蒸气电离度得到等离子体状态方程。考虑激光和等离子体的相互作用。进行了激光烧蚀铝靶的数值模拟,分析了靶的非稳态烧蚀过程。将计算结果与实验数据进行比较,比较了激波传播速度和压缩空气厚度,验证了计算方法的正确性。结果表明,冲击波演化具有复杂的结构,具有多密度的不连续性。在爆炸波的演变过程中,波前从早期的半椭圆形变为半球形,并且峰值密度位置从波前变为内部。激光作用下目标烧蚀率的波动范围(672 mJ,持续时间为24 ns)为0.08至0.32 mm / ns。等离子体密度分布与激光能量变化有关。激光脉冲后,等离子体的电离度和电子数密度先缓慢下降,然后急剧下降。

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