R. Cherdizov, V. Kokshenev, A. Shishlov, R. Baksht, Vladimir I. Oreshkin, A. Rousskikh, A. Zhigalin
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引用次数: 0
摘要
在托木斯克大电流电子学研究所的GIT-12发生器(4.7 MA, $1.7 \mu \ mathm {s}$)上,以2-3 MA的电流进行了外等离子体壳内爆金属膨胀Z钳的实验。外层等离子体外壳由48支等离子体枪组成,排列成直径35厘米的圆形。掐尖等离子体是由真空电弧在铝阴极和铝阳极之间的间隙中产生的。根据实验获得的电流和电压波形、磁探头信号以及条纹相机和HSFC Pro四帧光学相机拍摄的图像,估计了不同负载配置下产生的金属泡芙缩紧的初始质量密度分布。当半径R大于0.2 cm时,金属抽吸的初始径向质量密度分布近似为三个高斯函数。用密度均匀的铝等离子体射流形成R < 0.2 cm的掐痕中心部分。邻近喷射区(0.2 < R < 2 cm)的密度分布由真空电弧阳极铝离子的贡献提供。下一个密度分布(2 < R < 14 cm)可能是由真空电弧运行附近绝缘子表面的质量贡献决定的。等离子体枪在直径为35 cm处运行,在外围(14 < R < 16 cm)处出现密度峰值。
Estimation of the Al Metal-Puff Density Profile on the Generator GIT-12
Experiments on imploding metal-puff Z pinches with an outer plasma shell were performed at currents of 2–3 MA on the GIT-12 generator (4.7 MA, $1.7 \mu \mathrm{s}$) at the Institute of High Current Electronics (Tomsk). The outer plasma shell was produced by 48 plasma guns arranged in a circle of diameter 35 cm. The pinch plasma was generated by a vacuum arc which operated in a gap between an aluminum cathode and an aluminum anode. The initial mass density profiles of metal-puff pinches generated in different load configurations were estimated from experimentally obtained current and voltage waveforms, signals of magnetic probes, and images taken with a streak camera and an HSFC Pro four-frame optical camera. For radii $R$ larger than 0.2 cm, the initial radial mass density profile of a metal-puff pinch was approximated by three Gauss functions. The central part of the pinch with R < 0.2 cm was formed by an aluminum plasma jet with a uniform density. The density profiles in the adjacent jet region (0.2 < R < 2 cm) were provided by the contribution of the aluminum ions from the vacuum arc anode. The next density profile (2 < R < 14 cm) was probably determined by the mass contribution from the surface of the insulator near which the vacuum arc operated. The density peak at the periphery (14 < R < 16 cm) occurred due to the operation of the plasma guns at the diameter of 35 cm.