水中脉冲放电的时间发射特性

Xinpei Lu, M. Laroussi, J. Kolb, S. Kono, K. Schoenbach
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引用次数: 5

摘要

将高能脉冲动力系统从实验室推向实际应用,需要开发紧凑、轻便的驱动器。为了减小高压元件的尺寸和重量,需要在高电应力下提高电介质的能量密度。因此,深入了解液体电介质的阻压和击穿特性可以优化能量存储。在液体介质中,当击穿发生时,会产生蒸汽泡,气泡先膨胀,后坍缩。这些气泡膨胀和崩溃的总时间决定了高压开关可以操作的重复率。本文采用Blumlein脉冲形成网络(PFN)和球平面电极结构对水中脉冲放电进行了研究。球形电极的直径为1.7 mm,电极之间的间隙距离为几百微米。利用成像光谱仪测量了击穿后紫外和可见光光发射的时间发展。击穿后辐射强度达到最大5ns。在此水平保持约100 ns,然后在10 ns时间尺度上光强下降到峰值的30%。在脉冲中发现电流为800 A。测量了等离子体在击穿后100 ns内的辐射谱。未观察到线辐射。测量的光谱被发现遵循黑体辐射定律。因此,通过将实测光谱与计算黑体辐射在不同温度下的光谱进行比较,确定了等离子体温度。发现它在1-2 eV范围内。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Temporal emission behavior of pulsed discharge in water
To move the high energy pulsed power systems from the laboratory to practice requires the development of compact lightweight drivers. To reduce the size and weight of high voltage components, increase in the energy density in dielectrics at high electric stress is required. Therefore, an in-depth understanding of the hold-off voltage and breakdown properties of liquid dielectrics can lead to the optimization of energy storage. When breakdown is initiated in liquid dielectrics, vapor bubbles are generated, which first expand and later collapse. The total time of expansion and collapse of these bubbles determines the repetition rate at which high voltage switches can be operated. In this paper, a Blumlein pulse forming network (PFN) and sphere-plane electrode configuration is used for studying a pulsed discharge in water. The diameter of the spherical electrode is 1.7 mm and the gap distance between the electrodes is several hundred micrometers. The temporal development of the optical emission in the UV and visible after breakdown was measured by means of an imaging spectrograph. The radiation intensity reaches its maximum 5 ns after breakdown. It remains at this level for about 100 ns, and then the light intensity decreases to 30% of its peak value on a 10 ns time scale. The current was found to be 800 A during the pulse. The radiation spectrum of the plasma in the bubble during the 100 ns after breakdown was also measured. No line radiation was observed. The measured spectrum was found to follow a blackbody radiation law. Therefore by comparing the measured spectrum with that of calculated blackbody radiation at different temperatures, the plasma temperature was determined. It was found to be in the 1-2 eV range.
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