硅砂中聚合物圆柱体安装电弧电压上升机理的探讨

N. Kodama, Y. Yokomizu, Koya Nakamura, Asato Takahashi, Y. Kondo
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摘要

本报告描述了三个实验的直流中断实验结果:(1)硅砂填充(名称:Silica),(2)不填充硅砂的聚合物圆柱体安装(名称:P5-Air),(3)硅砂填充的聚合物圆柱体安装(名称:P5-Silica)。聚合物圆柱体的形状固定为内径5mm,长度为15mm。将峰值电流为750a的阻尼直流电输入到已建立的实验系统中。在供电期间,测量电极之间的电流和电压。实验结果表明,在峰值电流下,二氧化硅电极间的电弧电阻分别为0.15 Ω, P5-Air电极间的电弧电阻为0.20 Ω, p5 -二氧化硅电极间的电弧电阻为0.56 Ω。这意味着硅砂被限制在聚合物圆柱体中,有效地促进了电弧电压在峰值电流附近的上升。在电流衰减期间,p5 -空气的电弧电阻测量值与p5 -二氧化硅的电弧电阻几乎相同。这也意味着聚合物和电弧之间的相互作用在电流衰减期间提高了电弧电阻。
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Approach to Mechanism Interpretation of Arc Voltage Rise by Polymer Cylinder Installation in Silica-Sand
This report describes experimental results on DC interruption for three experiments: (1) silica-sand filling (designation: Silica), (2) polymer cylinder installation without silica-sand filling (designation: P5-Air), and (3) polymer cylinder installation with silica-sand filling (designation: P5-Silica). The shape of polymer cylinder was fixed at an inner diameter of 5 mm and a length of 15 mm. A damping DC with a peak current of 750 A was supplied to an established experimental system. A current and a voltage between electrodes were measured during the current supplying period. As experimental results, the arc resistance between electrodes were measured to be 0.15 Ω for Silica, 0.20 Ω for P5-Air and 0.56 Ω for P5-Silica at a peak current, respectively. This implies that silica-sand confined in the polymer cylinder effectively contributes to the arc voltage rise at around a peak current. During a current decaying periods, the arc resistance for P5-Air was measured to be almost same value for P5-Silica. This also implies that an interaction between the polymer and the arc rises the arc resistance during the current decaying period.
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