粘性流体中平行电极内运动粒子的电荷

K. Yatsuzuka, C. Choi, K. Asano
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引用次数: 10

摘要

在均匀电场作用下,粘性流体(硅油)中的导电球形颗粒表现为上下运动和运动间隙停留在电极上。为了从理论上分析导电粒子在电场作用下的运动,必须知道粒子的电荷量。它可以通过几种方法来实现。当导电粒子在电极上经历均匀场时,球形粒子的电荷量有一个众所周知的方程。第二种方法是利用动力学方程估计在粘性流体运动中作用于粒子的静电力。第三种方法是在粒子和电极之间发生电荷交换过程时集成脉冲电流。通过对电流积分得到的粒子电荷值要比其他方法小得多。电流脉冲宽度小于100 /spl mu/s,比静息时间短得多。这表明,从脉冲积分中获得的电荷可能不是整个电荷,但在粒子停留在电极上的时间内,可能会有几个小的放电跟随第一个放电。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the charge of a moving particle within a parallel electrodes in viscous fluid
The conductive spherical particle in viscous fluid (silicone oil) under a uniform electric field shows both up-and-down motion and resting on the electrode between motions. In order to analyze the motion of a conductive particle under electric field theoretically, the charge amount of particle must be known. It can be achieved with several methods. When the conductive particle is on the electrode experiencing the uniform field, there is a well-known equation for the charge amount of a spherical particle. The second way is to estimate the electrostatic force acting on the particle in the motion through viscous fluid by using dynamic equation. The third method is to integrate a pulsed current when the charge exchange process is occurring between the particle and the electrode. The value of particle charge by integrating the current is much smaller than the others. The width of the current pulse is less than 100 /spl mu/s, which is much shorter than the resting time. This suggests that the acquired charge from the integration of pulse might not be the whole charge, but several small discharges might follow the first one during the time the particle is resting on the electrode.
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