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Experimental investigation of the low‐frequency capacitive response of a plasma sheath

机译:等离子护套低频电容响应的实验研究

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摘要

Several theoretical models are examined for the low‐frequency capacitive response of the ion sheath surrounding both planar and cylindrical Langmuir probes in a collisionless plasma. It is found that a recent theoretical approach by Shkarofsky, based on the total probe surface charge derived from Gauss''s law, predicts values for both the low‐frequency, capacitance and the transient charge flow which are as much as an order of magnitude smaller than that predicted based on the electron current flow caused by the motion of the sheath edge, e.g., Kamke and Rose. This discrepancy is attributed to the neglect by Shkarofsky of the transient ion conduction current through the sheath. Additionally, a recent theory by Rosa for the complex impedance of a planar sheath is seen, in the limit of low frequency, to be in agreement with that predicted following Kamke and Rose. Experimental measurements have been made, for both pulsed and rf‐driven probes, of the transient charge flow to the probe and the effective low‐frequency sheath capacitance. These measurements show good agreement with the theoretical approach of Kamke and Rose, and Rosa. The plasma was formed in the positive column of a low‐pressure helium dc discharge with plasma electron densities and temperatures in the ranges 5 × 1015 -3 × 1016 m-3 and 5 × 105 -7 × 105 °K, respectively. The pulsed probe measurements were made by integrating the probe current response to both small‐ and large‐amplitude negative voltage pulses. The rf measurements were made using a tunnel diode oscillator circuit whose resonant frequency was chosen somewhat below the ion plasma frequency.
机译:针对无碰撞等离子体中围绕平面和圆柱形Langmuir探针的离子鞘的低频电容响应,研究了几种理论模型。我们发现,Shkarofsky最近的一种理论方法是基于高斯定律得出的总探头表面电荷,预测低频,电容和瞬态电荷流的数值都高达一个数量级。小于根据由鞘边缘(例如,坎克和罗斯)的运动引起的电子流预测的结果。这种差异归因于Shkarofsky忽略了通过护套的瞬态离子传导电流。另外,在低频范围内,Rosa提出的关于平面护套复阻抗的最新理论与在Kamke和Rose之后的预测相一致。对于脉冲探头和rf驱动探头,已经进行了实验测量,测量了流入探头的瞬态电荷和有效的低频护套电容。这些测量结果与Kamke和Rose和Rosa的理论方法非常吻合。等离子体在低压氦气直流放电的正极中形成,等离子体电子密度和温度分别在5×1015 -3×1016 m-3和5×105 -7×105°K范围内。脉冲探针测量是通过对小振幅和大振幅负电压脉冲的探针电流响应进行积分来进行的。使用隧道二极管振荡器电路进行射频测量,其谐振频率选择为略低于离子等离子体频率。

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    《Journal of Applied Physics》 |1973年第10期|共7页
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  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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