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Numerical study on space-charge-limited bipolar current flow in spherical electron sheath

机译:球形电子鞘中受空间电荷限制的双极性电流的数值研究

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Effect of bipolar current flow on the characteristics of spherical electron sheath has been studied by numerically solving Poisson's equation with iterative process. Contrary to the previous studies, simulations include not only the double layer, but also the transition state of the electron sheath with bipolar current flow. Simulation results show that the bipolar current flow due to the introduction of ion current increases the space-charge-limited electron current between fixed boundaries, owing to partial neutralization. The ratio of electron current increment depends on both radius ratios of outer to inner spheres and the fraction of ion to electron current. The maximum value of this ion current fraction, the Langmuir condition, is found to be proportional to the radius ratio and higher than the value of planar sheath. Correspondingly, maximum ratios of the electron current increment in spherical boundary are higher than that in planar electron sheath, 1.86. Based on the current enhancement at the fixed spherical boundary, increase of sheath thickness by the bipolar current flow is determined for the spherical electron sheath with movable boundary, considering area expansion of the sheath boundary. Depending on the initial boundary sphere radius ratios, sheath thickness increases until the ion current fraction reaches to the Langmuir condition. A remarkable result is that the maximum increment ratios of sheath thickness are identical to 1.364, the value of the planar sheath, regardless of the initial sheath thickness and boundary radius ratio. Since the current density, which determines the thickness of the electron sheath at fixed sheath voltage, is limited by the plasma properties, the sheath expansion ratio might be expected to be the same at fixed plasma condition, regardless of sheath geometry. This study will help to understand transition of spherical electron sheath to spherical double layer in the presence of bipolar current flow more clearly.
机译:通过用迭代过程对泊松方程进行数值求解,研究了双极性电流对球形电子鞘层特性的影响。与先前的研究相反,模拟不仅包括双层,还包括具有双极性电流的电子鞘的过渡态。仿真结果表明,由于部分中和,由于离子电流的引入而产生的双极电流增加了固定边界之间的空间电荷限制电子电流。电子电流增量的比率取决于外球与内球的半径比率以及离子对电子电流的比例。发现该离子电流分数的最大值(朗缪尔条件)与半径比成正比,并且高于平面护套的值。相应地,球形边界中电子电流增量的最大比率高于平面电子鞘中的最大比率1.86。基于在固定球面边界处的电流增强,考虑到鞘面边界的面积扩展,确定了具有可移动边界的球形电子鞘管由于双极电流而增加的鞘管厚度。取决于初始边界球半径比,护套厚度会增加,直到离子电流分数达到Langmuir条件为止。一个显着的结果是,无论初始护套厚度和边界半径比率如何,护套厚度的最大增量比率都等于1.364(平面护套的值)。由于决定了固定鞘管电压下电子鞘管厚度的电流密度受等离子体性能的限制,因此,无论鞘管的几何形状如何,在固定的等离子体条件下,鞘管的膨胀率都有望相同。这项研究将有助于更清楚地了解在存在双极性电流的情况下球形电子鞘向球形双层的转变。

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