Difference of Discharge Phenomena under GFRP and CFRP Insulation Barrier with Steep Impulse Voltage

N. Tanaka, D. Aoyagi, R. Sasamoto, Y. Izawa, K. Nishijima
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引用次数: 3

Abstract

Recently, many researchers focus on glass fiber reinforced plastic (GFRP) and carbon fiber reinforced plastic (CFRP) materials because these materials have superior mechanical properties. Therefore, their electrical insulation performance must be revealed. Especially, the discharge which occurred under insulation barriers has not been revealed. So, we have investigated the discharge phenomena under GFRP and CFRP insulation barriers. In this study, we used a needle-plane short air gap in the discharge chamber. The insulation barrier was placed 2 mm below the brass needle electrode and 5 mm above the plane electrode. Synthetic air (N2 (79%)/O2 (21%)) or room air was injected into the chamber at atmospheric pressure. The steep impulse voltages were repeatedly applied to the needle electrode. As a result, the surface discharge (SD), it developed in both gases on GFRP insulation barrier. However, it didn't develop on CFRP insulation barrier. Regarding the discharges under GFRP insulation barrier (barrier-plane discharges: BPDS), they mainly appeared in its center area at synthetic air. On the other hand, the discharges under CFRP insulation barrier appeared in overall area at both gases. In addition, the discharges were not occurred with the standard lightning impulse voltage.
冲击电压大时GFRP与CFRP绝缘屏障放电现象的差异
近年来,由于玻璃纤维增强塑料(GFRP)和碳纤维增强塑料(CFRP)材料具有优异的力学性能,引起了人们的广泛关注。因此,必须揭示其电绝缘性能。特别是在绝缘屏障下发生的放电没有被揭示出来。因此,我们对GFRP和CFRP绝缘屏障下的放电现象进行了研究。在本研究中,我们在放电室内采用针平面短气隙。绝缘屏障放置在铜针电极下方2mm,平面电极上方5mm。在常压下将合成空气(N2 (79%)/O2(21%))或室内空气注入腔内。在针电极上反复施加陡峭的脉冲电压。因此,表面放电(SD),它发展在两种气体的GFRP绝缘屏障上。但在CFRP绝缘屏障上没有得到发展。玻璃钢绝缘屏障下的放电(障面放电:BPDS)主要出现在合成空气处的屏障中心区域。另一方面,CFRP保温屏障下的放电在两种气体的总体面积上都出现了。此外,在标准雷击电压下,不发生放电。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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