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The Edge Effect on the EEDF Measurements ofMagnetized DC Plasma

机译:磁化直流等离子体的EEDF测量的边缘效应

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The localized plasma parameters at the edge of the discharge electrodes cell have been investigated for axial distribution, such as the electric field distribution, the electron energy distribution functions (EEDF), the electron temperature (Te) and the electron density (Ne), all have been determined with and without the applications of external magnetic field using Langmuir single probe in the three regions of the discharge. The EEDF was investigated using two different methods e.g. the graphical method and the electron current second derivative method. The electron energy distribution functions are maxwellian only in the positive column region (P.C.) and non- maxwellian in the cathode fall (C.F) and the negative glow (N.G.) regions, where two groups of electrons were observed. The diffusion coefficients and the electron temperatures are lower in the presence of the magnetic field, where Te decreased from 6.5 to 3 eV for C.F, from 5.18 to 2.6 eV for N.G., and from 4.2 to 1.1 eV for P.C. Furthermore, sharp axial increments for potential distribution and electron density in the presence of the magnetic field were measured, whereas in the border between C.F and N.G regions, Ne increased from 4 x109 to 9.5 x109 cm-3 and 4.97 x109 to 11.6 x109 cm-3, respectively. In contrast, an axial decrement of the electron density in P.C. region due to the electron capture by the anode in P.C. region was also found.
机译:已经研究了放电电极单元边缘的局部等离子体参数的轴向分布,例如电场分布,电子能量分布函数(EEDF),电子温度(Te)和电子密度(Ne),所有在放电的三个区域中使用朗缪尔单探针确定了有无外部磁场的作用。使用两种不同的方法对EEDF进行了研究,例如图形方法和电子电流二阶导数方法。电子能量分布函数仅在正列区域(P.C.)中为麦克斯韦,在阴极下降(C.F)和负辉光(N.G.)中为非麦克斯韦,其中观察到两组电子。在磁场存在下,扩散系数和电子温度较低,其中Te从C.F从6.5降至3 eV,从N.G.从5.18降至2.6 eV,从P.C从4.2降至1.1 eV。此外,测量了在磁场存在下电位分布和电子密度的急剧轴向增量,而在CF和NG区域之间的边界,Ne从4 x109增大到9.5 x109 cm-3,从4.97 x109增大到11.6 x109 cm- 3,分别。相反,在P.C中,电子密度沿轴向减小。由于P.C中的阳极会捕获电子,因此该区域还发现了该地区。

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