电流蒙皮方式下电导体爆炸的实验研究

N. Labetskaya, V. Oreshkin, S. Chaikovsky, I. Datsko, Y. A. Sukovatitsyn, E. Volkov
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引用次数: 1

摘要

研究不同金属表面在磁感应率上升至1011 T/s时的等离子体形成,对提高多兆安脉冲发电机真空传输线的能量传输效率具有重要意义。这种具有z箍缩辐射负载的发生器是实现惯性约束核聚变的候选者。导体表面等离子体的形成是由于电流蒙皮模式下的电爆炸引起的。在这种模式下,输入导体的能量的时间小于磁场的扩散时间。从兆赫斯磁场的微秒实验中,我们知道导体的破坏发生在磁感应强度为几兆赫斯的磁场中。在快速上升的超高斯磁场中,等离子体形成的实验数据非常有限。因此,在MIG脉冲电源发生器上(电流2.5 MA,上升时间100 ns),在导体表面磁场上升速率(0.8÷1.5)·1010 T/s的电流蒙皮模式下圆柱形导体的爆炸实验。由铝、铜和钛制成的导体直径为(1÷3.5) mm,用真空紫外辐射探测器记录了导体表面等离子体形成的瞬间。我们得出结论,在目前的蒙皮模式下,磁感应度存在某个阈值,这是磁能密度足够接近材料升华能时的值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Experimental research of electrical conductor explosion in the current skinning mode
The research of plasma formation on the surface of different metals at the rise rate of the magnetic induction up to 1011 T/s is of interest in terms of energy transport efficiency in the vacuum transmission lines of multi-megaampere pulsed power generators. Such generators with a Z-pinch radiating load are the candidates for realization of inertial confinement fusion. The formation of plasma on the conductor surface occurs due to the electrical explosion in the current skinning mode. In this mode the time of the energy input into a conductor is less than the diffusion time of the magnetic field. From microsecond experiments with megagauss magnetic fields, it is known that the destruction of a conductor occurs in the field with magnetic induction of a few megagausses. The amount of available experimental data on plasma formation in fast-rising megegauss magnetic fields is very limited. Therefore, the experiments on the explosion of cylindrical conductors in the current skinning mode at the rise rate of magnetic field on the conductor surface of (0.8÷1.5)·1010 T/s were carried out on the MIG pulsed power generator (current 2.5 MA, rise time 100 ns). The diameters of conductors made of aluminum, copper and titanium were (1÷3.5) mm. The instant of plasma formation on the conductor surface was registered by detectors of vacuum ultraviolet radiation. We have concluded that in the current skinning mode the some threshold value of the magnetic induction exists and this is that value when the magnetic energy density is enough close to the sublimation energy of the material.
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