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首页> 外文期刊>IEEE Transactions on Plasma Science >Probe Measurement of Residual Plasma of a Magnetically Confined High-Current Vacuum Arc
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Probe Measurement of Residual Plasma of a Magnetically Confined High-Current Vacuum Arc

机译:磁约束大电流真空电弧的残余等离子体的探针测量

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摘要

The electron temperature and ion density of the residual plasma of a magnetically confined high-current vacuum arc were measured using the electrostatic (Langmuir) probe method. Measurements were performed in a triggered-vacuum gap using a 40-mm-diameter oxygen-free copper (OFCu) cathode and an anode of 100 mm diameter separated by a gap of 30 mm. The arc current is a sinusoidal wave having a half-period of approximately 1 ms and a peak value ranging from 1 to 5 kA. An axial magnetic field (AMF) was supplied by either a dc field coil or AMF-type electrodes, which generate an ac magnetic field in close proximity that has coincident phase with arc current. It was found that the electron temperature of the residual plasma did not depend on current peak, and current gradient and space remained in a constant range of 2.2-3.0 eV. The radial distribution of ion density was diffusive, in contrast to the parabolic confined distribution of the steady-state arc. The characteristics obtained for the dc magnetic field and those obtained for the AMF electrode were identical except for the ion density at current zero.
机译:使用静电(Langmuir)探针法测量磁约束的高电流真空电弧的残余等离子体的电子温度和离子密度。使用直径为40 mm的无氧铜(OFCu)阴极和直径为100 mm的阳极(间隔为30 mm)在触发真空间隙中进行测量。电弧电流是正弦波,半周期约为1 ms,峰值范围为1至5 kA。轴向磁场(AMF)由直流磁场线圈或AMF型电极提供,它们会在附近产生与电弧电流相位一致的交流磁场。发现残余等离子体的电子温度不取决于电流峰值,并且电流梯度和空间保持在2.2-3.0eV的恒定范围内。与稳态电弧的抛物线限定分布相反,离子密度的径向分布具有扩散性。除电流为零时的离子密度外,直流磁场获得的特性与AMF电极获得的特性相同。

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