...
首页> 外文期刊>Plasma Science, IEEE Transactions on >Anode Current Density Distribution Measurements for Different Vacuum Arc Modes Subjected to Axial Magnetic Field
【24h】

Anode Current Density Distribution Measurements for Different Vacuum Arc Modes Subjected to Axial Magnetic Field

机译:轴向磁场作用下不同真空电弧模式下阳极电流密度分布的测量

获取原文
获取原文并翻译 | 示例
           

摘要

We report our measurements of anode current density distributions for different modes in vacuum arc discharge using a split-anode and a cup-shaped axial magnetic field cathode configuration system. The modes investigated included the diffuse arc and anode spot. The anode surface was divided into four regions: one central region and three symmetrical-disposed peripheral annular-arc regions. Three different-sized central regions were selected with diameters of 12, 18, and 20 mm. The contact material was CuCr25 (25% Cr). The arc current in the tests ranged from 6 to 14 kA (rms) at 50 Hz. The opening velocities were 1.8 and 2.4 m/s, respectively. The currents of the four areas on the anode contact were measured by four Rogowski coils situated outside the vacuum chamber. The experimental results show the current density distribution in different arc modes. For the diffuse arc mode with arc currents of 6 and 8 kA (rms), the average current density in the central region at current peak ranged from 8.5 to 15.9 A/mm. The anode spot current density ranged from 31.9 to 37.7 A/mm, estimated from the current density in the eroded region caused by the anode spots covering the entire central region of diameters 12 and 18 mm, at currents of 12 and 14 kA, respectively, regarded as the lower limit current density of the anode spot. Moreover, the dependence of the current density distribution on opening velocity in diffuse arcs was slight. For the anode spots, the current density distribution with higher opening velocity was more concentrated.
机译:我们报告了使用分流阳极和杯形轴向磁场阴极配置系统在真空电弧放电中不同模式下阳极电流密度分布的测量结果。研究的模式包括扩散电弧和阳极点。阳极表面分为四个区域:一个中心区域和三个对称布置的外围环形弧区域。选择了直径为12、18和20毫米的三个不同大小的中心区域。接触材料是CuCr25(25%Cr)。测试中的电弧电流在50 Hz时范围为6至14 kA(rms)。开启速度分别为1.8和2.4 m / s。阳极触点上四个区域的电流由位于真空室外部的四个Rogowski线圈测量。实验结果表明了不同电弧模式下的电流密度分布。对于电弧电流为6和8 kA(rms)的扩散电弧模式,在中心区域的电流峰值处的平均电流密度为8.5至15.9 A / mm。阳极点电流密度范围为31.9至37.7 A / mm,这是根据在12和14 kA的电流下分别覆盖直径为12和18 mm的整个中心区域的阳极点引起的腐蚀区域中的电流密度估算得出的,视为阳极点的下限电流密度。而且,电流密度分布对弥散电弧中打开速度的依赖性很小。对于阳极点,具有较高打开速度的电流密度分布更加集中。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号