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Effect of an axial magnetic field and arc current on the anode current density in diffuse vacuum arcs

机译:轴向磁场和电弧电流对扩散真空电弧中阳极电流密度的影响

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The objective of this paper is to measure the effect of an axial magnetic field (AMF) B-AMF and arc current on the anode current density in diffuse vacuum arcs. The experimental geometry included a split anode and a butt-type cathode, both with a diameter of 60 mm. The anode surface was divided into a central area and three symmetrically disposed peripheral annular areas. The central area of the split anode had a diameter of 20 mm. The contact material was CuCr25 (25% Cr). The arc current IARC ranged from 4 to 14 kA (rms) at 50 Hz. The opening velocity was 2.4 m/s. The currents of the four areas on the anode contact were measured using four Rogowski coils situated outside the vacuum chamber. An external uniform AMF B-AMF ranging from 0 to 110mT was applied during the experiment. The observed arc modes were recorded by a high-speed charge-coupled device video camera. The experimental results quantitatively reveal that the current density distribution on the anode surface in the diffuse arc mode was not uniform but concentrated in the central area. The current density in the central anode area at the current peak J(Area I)(Peak) decreased with increasing B-AMF following a power law. For B-AMF of 0-110mT and I-ARC of 4-14 kA, J(Area I)(Peak) = (2.2 I-ARC + 0.069 I-ARC(2)) B-AMF -0.22, where J(Area I)(Peak) is in A/mm(2), B-AMF is in mT, and I-ARC is in kA. Moreover, the current distribution was uneven in the three peripheral areas. Published by AIP Publishing.
机译:本文的目的是测量轴向磁场(AMF)B-AMF和电弧电流对扩散真空电弧中阳极电流密度的影响。实验几何形状包括直径为60 mm的分体式阳极和对接式阴极。将阳极表面分为中心区域和三个对称设置的外围环形区域。分离阳极的中心区域的直径为20毫米。接触材料是CuCr25(25%Cr)。在50 Hz时,电弧电流IARC的范围为4至14 kA(rms)。打开速度为2.4m / s。使用位于真空室外部的四个Rogowski线圈测量阳极触点上四个区域的电流。在实验过程中使用了范围从0到110mT的外部均匀AMF B-AMF。观察到的电弧模式由高速电荷耦合器件摄像机记录。实验结果定量地表明,扩散弧模式下阳极表面的电流密度分布不​​均匀,而是集中在中心区域。遵循幂定律,随着B-AMF的增加,电流峰值J(A区)(Peak)处的阳极中心区域的电流密度降低。对于0-110mT的B-AMF和4-14 kA的I-ARC,J(面积I)(峰值)=(2.2 I-ARC + 0.069 I-ARC(2))B-AMF -0.22,其中J(面积I)(峰值)以A / mm(2)为单位,B-AMF以mT为单位,而I-ARC以kA为单位。此外,在三个外围区域的电流分布不均匀。由AIP Publishing发布。

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