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Interferometry Of Single And Double wire plasma radiation source loads

机译:单线和双线等离子体辐射源负载的干涉测量

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Models developed for the implosion of multi-wire arrays used as plasma radiation sources depend upon the assumption that the entire wire mass is ionized, forms a symmetric thin plasma shell and participates in the implosion process. Any deviation from this scenario in an actual experiment can lead to poor correlation between the model and experimental measurements at best or an incorrect picture of the real physics at worst. In order to address this problem, HY-Tech researchers are applying various time resolved interferometric techniques to study the evolution of plasmas from single and dual wire loads. One system employed uses a flashlanip pumped dye laser (approximately 300 ns pulse length) as a source and a gated, intensified framing/streak camera as the detector. Used in the framming mode, 20 ns snapshot-interferograms are produced giving a full view of the wire and surrounding plasma. Used in the streak mode, a radial view of the interferometer fringes (tirne resolved over the laser pulse) is produced for a given axial position on the wire thus providing a measure of the radial extent and motion of the wire plasma. In a separate system, single or double pulse, diffuse illumination holograms are produced with a ruby laser (10 ns pulse width). The double pulse hologram produces an interferogram upon reconstruction while the single pulse hologram reconstructs the original wavefront which can be post-processed using Schleiren or shadow techniques to highlight and measure plasma density gradients. Measurements will be presented showing the evolution of plasmas from single and dual wire loads.
机译:为内爆用作等离子体辐射源的多线阵列的内爆而开发的模型取决于以下假设:整个导线均被电离,形成对称的薄等离子壳体,并参与内爆过程。实际实验中与这种情况的任何偏离都可能导致模型与实验测量之间的相关性最差,或者最坏的情况是导致真实物理情况的不正确。为了解决这个问题,HY-Tech研究人员正在应用各种时间分辨干涉测量技术来研究单线和双线负载下等离子体的演变。使用的一种系统使用闪蒸泵浦的染料激光器(大约300 ns的脉冲长度)作为光源,并使用门控的增强成帧/条纹相机作为检测器。在成帧模式下使用时,会产生20 ns快照干涉图,从而可以看到导线和周围等离子的完整视图。在条纹模式下使用时,对于导线上的给定轴向位置,可以生成干涉仪条纹的径向视图(在激光脉冲上分辨出的三聚氰胺),从而提供了径向范围和导线等离子运动的度量。在单独的系统中,用红宝石激光器(10 ns脉冲宽度)产生单脉冲或双脉冲漫射照明全息图。双脉冲全息图在重建时会产生干涉图,而单脉冲全息图会重建原始波前,可以使用Schleiren或阴影技术对其进行后期处理,以突出显示和测量等离子体密度梯度。将提供测量结果,以显示单线和双线负载下等离子体的演变。

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