Analytical calculation of the point-to-point partial inductance of a perfect ground plane

Umberto Paoletti, T. Hisakado, Osami Wada
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引用次数: 3

Abstract

The point-to-point partial self inductance of an infinite and perfectly conducting ground plane has been analytically calculated in closed form. The point-to-point mutual coupling between ground plane and a trace parallel to the ground plane has been expressed in terms of an integral, which should be solved numerically. The calculations are based on a new scalar potential directly related to the concept of partial inductances. Formulas for the conversion of partial inductances between the Lorenz's and Coulomb's gauges are also obtained. The definition of partial inductance in terms of the vector potential (e.g. in [1]) implicitly introduces equivalent circuits, where the voltage represents a difference of a scalar potential defined by the electric field and by the magnetic vector potential at the same time. Therefore, it should not surprise the possibility of having a partial inductance also on perfect ground planes. A part from the definition of the magnetic vector potential, the definition of ground plane partial inductance depends on the application, in particular on the considered current distribution on the ground plane. For example, in [2] the ground plane inductance is defined in terms of the induced current on the ground plane by a micro-strip conductor. In the present work, we will consider the current injected in one point and extracted from a second point on the ground plane, similarly to [3]. This type of partial inductance appears when there are connections to a ground plane, such as cables or micro-strip terminations. In a less proper way, it can be used for approximately representing the inductance related to the displacement current, when a micro-strip is decomposed in short segments carrying constant current. The numerical calculation of the point-to-point ground partial inductance is already considered in software of widespread use, such as FASTHENRY [4]. However, the segmentation of the ground plane can become a problem for configurations with high density of conductors [5]. The calculation time increases for larger ground planes, also because the image theory cannot be directly applied to the calculation of partial inductances.
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完美地平面点对点局部电感的解析计算
以封闭形式解析计算了无限大完美导电地平面的点对点部分自感。地平面与平行于地平面的迹线之间的点对点相互耦合用积分表示,需要用数值方法求解。计算是基于一个新的标量电位直接相关的部分电感的概念。还得到了洛伦兹量规和库仑量规之间部分电感转换的公式。用矢量电势来定义部分电感(例如在[1]中)隐含地引入了等效电路,其中电压表示由电场和磁矢量电势同时定义的标量电势的差。因此,在完美的接地面上也有部分电感的可能性就不足为奇了。一部分从磁矢量电位的定义出发,地平面部分电感的定义取决于应用场合,特别是考虑地平面上的电流分布。例如,在[2]中,地平面电感根据微带导体在地平面上的感应电流来定义。在本工作中,我们将考虑在一个点注入电流,并从地平面上的另一个点提取电流,类似于[3]。这种类型的部分电感出现在有连接到地平面,如电缆或微带端子。在一种不太合适的方式下,它可以用来近似表示与位移电流有关的电感,当微带被分解成带有恒定电流的短段时。在FASTHENRY[4]等广泛使用的软件中,已经考虑了点对点地偏电感的数值计算。然而,对于高密度导体的配置,地平面的分割会成为一个问题[5]。对于较大的地平面,计算时间增加,这也是因为像理论不能直接应用于局部电感的计算。
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On relative error minimization in passivity enforcement schemes Measurement of interconnect loss due to dummy fills Analytical calculation of the point-to-point partial inductance of a perfect ground plane Removing redundancy in interconnect simulation using domain decomposition techniques Fast calculation of PEEC macromodels using frequency derivatives
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