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Electrostatic proximity force, toner adhesion, and atomic force microscopy of insulating particles

机译:静电接近力,墨粉附着力和绝缘颗粒的原子力显微镜

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摘要

It has recently been shown [Czarnecki and Schein, J. Electrostat. 61 (2004) 107] that the electrostatic adhesion of a discrete distribution of charge points that are symmetrically distributed around a sphere in contact with a conductive plane is larger than the conventional result, (1/4 pi epsilon(0))(Q(2)/4r(2)), (which describes the adhesion of a spherically symmetric charge distribution to a conductive plane) by (1 + 4/pi) where Q is the total charge and r is the radius of the spherical particle. This is a surprising result since it is conventionally assumed that a charged insulating particle can be modeled as a spherically symmetric charge distribution which is equivalent to a single charge point Q located in the center of the sphere. This new electrostatic force, the 4/pi term which is due to quantized nature of charge, is called the electrostatic proximity force. Previously published, poorly understood toner adhesion data and atomic force microscopy experiments with insulating particles can be accounted for using the proximity force. (c) 2005 Elsevier B.V. All rights reserved.
机译:最近显示了它[Czarnecki和Schein,J。Electrostat。 61(2004)107]认为,与导电平面接触的球体周围对称分布的电荷点的离散分布的静电粘附力大于传统结果,(1/4 pi epsilon(0))(Q( 2)/ 4r(2)),(描述球形对称电荷分布在导电平面上的附着力)乘以(1 + 4 / pi),其中Q为总电荷,r为球形颗粒的半径。这是令人惊讶的结果,因为通常认为带电的绝缘粒子可以建模为球形对称的电荷分布,等效于位于球心的单个电荷点Q。这种新的静电力(由于电荷的量化性质而导致的4 / pi项)称为静电接近力。以前发表的,理解不充分的墨粉附着力数据和使用绝缘粒子的原子力显微镜实验可以解释为使用接近力。 (c)2005 Elsevier B.V.保留所有权利。

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