真空电弧放电形成的金属雾化等离子体射流的射线照相研究

A. Rousskikh, A. Artyomov, A. Zhigalin, A. Fedunin, V. Oreshkin, R. Baksht
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引用次数: 0

摘要

目前,除了线阵和气吹式z -夹紧外,还使用了Metal-Puff z -夹紧(基于真空电弧放电系统)[1]。Metal-Puff Z-pinch的优点是:A -显著的初始电导率(~ 104欧姆−1-m−1[2]),因此,没有“冷启动”的问题,B -可重复使用的可能性和C -稳定的Z-pinch内爆。衬垫壳体最重要的参数之一是物质分布(沿其长度和横向)。研究致密等离子体流分布的最有效方法是X-pinch射线摄影(空间分辨率约为10 μm,而时间分辨率约为1 ns[3])。该诊断装置与用与所研究等离子体相同的材料制造的阶梯楔相结合,不仅可以对等离子体流动结构进行定性分析,还可以进行定量分析。本工作的主要目的是确定不同几何形状等离子体射流形成时单位长度等离子体射流质量的分布。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Radiographic research of the metal-puff plasma jets formed by the vacuum arc discharge
Currently, along with the wire array and gas-puff Z-pinches, the Metal-Puff Z-pinches (based on vacuum arc discharge systems) are used [1]. The advantages of Metal-Puff Z-pinches are: A — significant initial conductivity (~ 104 Ohm−1-m−1 [2]) and consequently, the absence of a problem with a “cold start”, B — possibility of reusable use and C — stable Z-pinch implosion. One of the most important parameters of the liner shell is the substance distribution (both across and along its length). The most informative method for investigation of the dense plasma stream distribution is X-pinch radiography (the spatial resolution is about of 10 μm, while the temporal resolution is about of 1 ns [3]). The diagnostics in combination with the step-wedge manufactured from the same material as the investigated plasma, allows carrying out not only qualitative but also quantitative analysis of the plasma flow structure. The main aim of the work was to determine the distribution of the plasma jet mass per unit length for different geometry of the plasma jet formation.
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