单线电极接触ABD对能量沉积的影响

C. Myers, P. Schrafel, D. Chalenski, B. Kusse
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引用次数: 0

摘要

只提供摘要形式。当单根导线被短而大电流的脉冲驱动时,当沿导线形成日冕等离子体时,所沉积的能量会因电压崩溃而终止。已经证明,这种等离子体的形成和沉积的能量会受到电线和电极之间建立电接触的方式的影响。研究还表明,焊接触点或改进的机械触点可以延缓等离子体的形成,增加沉积能量。我们在这里提出了更详细的实验,使用一种新的方法来改善电线和电极之间的电连接。大直径,50mum, 5056铝线被化学蚀刻到25mum,除了在线电极接触发生的末端区域。确定了初始导线直径,并使用衍射技术调整了电极之间的位置。小心翼翼地使电线较粗的部分延伸到阳极-阴极间隙区域被最小化。使用这些类型的导线在电压崩溃前沉积的能量与使用简单机械电极触点的均匀直径25 μ m导线沉积的能量以及使用焊接触点的25 μ m导线沉积的能量进行了比较。类似的实验计划从更大的电线开始,例如75和100微米。利用532纳米激光干涉测量技术,对导线两端靠近电极的等离子体进行了详细的随时间变化的测量。利用时间相关的激光背光来观察电压崩溃后导线的膨胀。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Single Wire Electrode Contacts ABD their Effects on Energy Deposition
Summary form only given. When single wires are driven with short, high-current pulses the energy deposited is terminated by a voltage collapse that occurs when coronal plasma forms along the wire. It has been shown that the formation of this plasma and the amount of energy deposited can be affected by the way electrical contact is established between a wire and the electrodes. It has also been shown that soldered contacts or improved mechanical contacts can delay the plasma formation and increase the energy deposited. We present here more detailed experiments using a new approach for improving the electrical connection between the wires and electrodes. Large diameter, 50 mum, 5056 aluminum wires were chemically etched down to 25 mum except for regions at the ends where the wire-electrode contact occurred. Initial wire diameters were determined and placement between the electrodes was adjusted using diffraction techniques. Care was taken so that the extension of the thicker portion of the wires into the anode-cathode gap region was minimized. Energy deposited before voltage collapse using these types of wires was compared to the energy deposited in uniform diameter 25 mum wires with simple mechanical electrode contacts and also with 25 mum wires using soldered contacts. Similar experiments are planned starting with larger wires of, for example 75 and 100 mum. Detailed time dependent measurements of the plasma at the ends of the wires, near the electrodes, was made using 532 nm laser interferometry. Time dependent laser backlighting was used to observe the wire expansion after the voltage collapse.
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