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Arc Appearance and Cathode Spot Distribution in a Long-Gap High-Current Vacuum Arc Controlled by an External Axial Magnetic Field

机译:外部轴向磁场控制的长间隙大电流真空电弧的电弧外观和阴极斑点分布

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An experimental study of a high-current vacuum arc generated between two static CuCr25 contacts spaced 20 or 30 mm apart was conducted to characterize the arc appearance and the cathode spot (CS) distribution. The arc was ignited from the lateral surface of the cathode and controlled using an external axial magnetic field. Under the investigated experimental conditions, three distinct arc modes have been observed: multiple arc, diffuse, and diffuse columnar modes. The latter appeared at low BAMF/Iarcvalues, typically below 4 mT/kA. The temporal evolutions of the spot spatial distribution and the associated distribution of the current density were analyzed by processing high-speed video images of the cathode. Various types of distribution depending mainly on current were identified. At low currents (up to 13 kA), the CS distribution covered only a fraction of the cathode surface. At intermediate currents (in 17.2-31.1-kA range), CSs were present on the whole circumference of the cathode and the CS distribution included a closed region without spot. The latter was progressively filled by CSs, yet it totally disappeared before the end of arcing only when its location was off-centered with respect to the cathode axis. At high currents (up to 36.3 kA), the whole cathode surface was occupied by CSs at current peak. The azimuthally averaged radial distribution of the current density was found to be relatively uniform in the regions occupied by CSs. An average spot current of 36.5 ± 2.5 A has been estimated.
机译:对两个间隔20或30 mm的静态CuCr25触点之间产生的大电流真空电弧进行了实验研究,以表征电弧外观和阴极斑点(CS)分布。从阴极的侧面点燃电弧,并使用外部轴向磁场控制电弧。在研究的实验条件下,已观察到三种不同的电弧模式:多重电弧,扩散和扩散柱状模式。后者出现在较低的B n AMF n / I n arc值,通常低于4 mT / kA。通过处理阴极的高速视频图像,分析了光点空间分布的时间演变以及电流密度的相关分布。确定了主要取决于电流的各种类型的分布。在低电流(高达13 kA)下,CS分布仅覆盖阴极表面的一小部分。在中等电流下(在17.2-31.1-kA范围内),CSs存在于阴极的整个圆周上,并且CS分布包括没有斑点的封闭区域。后者逐渐被CS填充,但只有在其位置相对于阴极轴偏离中心时,它才在电弧放电结束之前完全消失。在大电流(高达36.3 kA)下,整个阴极表面在电流峰值处被CS占据。发现电流密度的方位角平均径向分布在CS占据的区域中相对均匀。估计平均点电流为36.5±2.5A。

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