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首页> 外文期刊>Electrical engineering in Japan >Measurements of Electron Density and Electron Temperature of Arc Discharge Plasmas Containing Metallic Vapors Using Laser Thomson Scattering
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Measurements of Electron Density and Electron Temperature of Arc Discharge Plasmas Containing Metallic Vapors Using Laser Thomson Scattering

机译:激光汤姆森散射法测量含金属蒸气的电弧放电等离子体的电子密度和电子温度

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摘要

Laser Thomson scattering (LTS) was applied to arc discharges generated in the atmosphere to measure electron density (n_e) and electron temperature (T_e). The electrode gap was 0.8 mm, and the electrode diameter was 1 mm. The applied voltage was 6 kV, the peak current was 600 A, and the decay time of the voltage and current was 25 μs. The spatiotemporal evolution of n_e and T_e was measured 10, 30, and 50μs after discharge initiation. At these times, the obtained values of n_e and T_e were estimated to be in the ranges of (0.8 to 2.0) × 10~(23) m~(-3) and 1.0 to 2.2 eV, respectively. These values were consistent with those evaluated using Saha's thermodynamic equation at 1 atm. It was also found that the decay of the arc discharge produced using the tungsten-copper electrodes was much faster than that produced using the tungsten electrodes.
机译:将激光汤姆森散射(LTS)应用于大气中产生的电弧放电,以测量电子密度(n_e)和电子温度(T_e)。电极间隙为0.8mm,电极直径为1mm。施加的电压为6 kV,峰值电流为600 A,电压和电流的衰减时间为25μs。放电开始后10、30和50μs测量n_e和T_e的时空演变。此时,估计得到的n_e和T_e的值分别在(0.8至2.0)×10〜(23)m〜(-3)和1.0至2.2eV的范围内。这些值与在1个大气压下使用Saha热力学方程评估的值一致。还发现使用钨铜电极产生的电弧放电的衰减比使用钨电极产生的电弧放电的衰减快得多。

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