激光诱导荧光法诊断真空电弧中铜蒸气的二维分布

Jiankun Liu, Ziru Zha, Zhenxing Wang, Liqiong Sun, Jianhua Wang, Yingsan Geng, Zhiyuan Liu
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引用次数: 0

摘要

为了更好地理解真空断弧过程,获得电弧过程中中性金属蒸气的信息是非常重要的。在这项工作中,目的是实验研究在电弧过程中铜蒸气的二维分布。在特定的时间点注入反向电流,迫使45 Hz的正弦电弧电流在短时间内熄灭,避免了强烈的电弧自辐射干扰。同时,采用中心波长为324.8 nm的脉冲激光平面激光诱导荧光(PLIF)激发金属蒸气,用iCCD相机记录了诱导荧光产生的金属蒸气的分布。实验采用了一对杯形轴向磁场触点。材料为CuCr50,电弧电流峰值幅值为3 kA。结果表明,金属蒸气密度峰值出现在8 ms左右,电流峰值出现在3 ms左右,密度最大值可达2.3×1020m-3。同时发现,电弧过程中金属蒸气主要积聚在阳极表面,当电流开始下降时,这种现象变得明显。
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Two Dimensional Distribution Diagnostic of Copper Vapor in a Vacuum Arc by Laser-induced Fluorescence
It is important to obtain the information on the neutral metallic vapor during the arcing period for a better understanding of vacuum arc interruption process. In this work, the objective is to experimentally study the two dimensional distribution of copper vapor during arcing. A reverse current was injected at specific time points to force the 45 Hz sinusoidal arc current to be extinguished in a short time, avoiding the interference of intensive arc self-radiation. Meanwhile, the plane laser-induced fluorescence (PLIF) using a pulse laser with a central wavelength at 324.8 nm was adopted to excite the metallic vapor, and a iCCD camera recorded the distribution of the vapor from the induced fluorescence. In the experiments, a pair of cup-shaped axial magnetic field (AMF) contacts were used. The material was CuCr50 and the peak amplitude of the arc current was 3 kA. It is found that the peak value of the metallic vapor density occurred at about 8 ms while the current peak occurred approximate 3 ms in advance, and the highest density value can achieve up to 2.3×1020m-3. It is also found that the metallic vapor mainly accumulated on the anode surface under AMF during the arcing period, which became obvious when the current begins to drop.
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