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Effective constriction resistance for isotropic and anisotropic film conductors

机译:各向同性和各向异性膜导体的有效收缩性

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摘要

When two electrical conductors with rough surfaces are in contact, the apparent contact area can be regarded as an ensemble of small real contact spots, as noted by Holm. The currents flowing through a real contact spot are influenced by the electrical current spread from the adjacent real contact spots. Greenwood considered the interference between a pair of real contact spots. The effective constriction resistance thus obtained can be evaluated once the positions of the real contact spots have been determined. For decades, the expressions for the constriction resistance obtained by Holm and Greenwood have been widely used to interpret and characterize experimental data. Here, we take a completely different approach. Instead of explicitly considering the interference between the real contact spots using their specific positions, we regard the apparent contact area composed of an ensemble of real contact spots as a homogeneous effective conductor. The effective medium theory is not rigorous but its simplicity allows us to study the effective constriction resistance of film and bulk conductors, including the effect of conductivity anisotropy, approximately. We show that the obtained effective resistance is consistent with that obtained by Greenwood for bulk isotropic conductors. We also propose a phenomenological equation to describe the relation between the Holm radius and the number of real contact spots.
机译:当两个表面粗糙的导电体接触时,表观接触面积可被视为小的真实接触点的集合,如Holm所述。流经真实接触点的电流受到来自相邻真实接触点的电流传播的影响。格林伍德考虑了一对真实接触点之间的干扰。一旦确定了实际接触点的位置,就可以评估由此获得的有效收缩阻力。几十年来,Holm和Greenwood获得的收缩阻力表达式已被广泛用于解释和表征实验数据。在这里,我们采取了完全不同的方法。我们没有使用实际接触点的特定位置来明确考虑实际接触点之间的干扰,而是将由实际接触点集合组成的表观接触面积视为均匀有效导体。有效介质理论并不严格,但它的简单性使我们可以近似地研究薄膜和体导体的有效收缩电阻,包括电导率各向异性的影响。我们表明,获得的有效电阻与Greenwood获得的体各向同性导体的有效电阻一致。我们还提出了一个唯象方程来描述霍姆半径和实际接触点数量之间的关系。

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