2003•Unpublished venueRequires access

Enhanced skin effect for partial element equivalent circuit (PEEC) models

K.M. Coperich, A.E. Ruehli, Andreas C. Cangellaris

Open publisher page 20 citations

Abstract

A convenient skin effect model for the partial element equivalent circuits (PEEC) technique is the so-called volume filament technique. This approach is an integral part of the basic PEEC model if the conductor cross-sections are subdivided into cells. This model is efficient for geometries and frequencies where the skin depth is moderate compared to the conductor thickness. However, the computational cost may be too high for the case where the skin depth is a small fraction of the cross-section, especially if it is subdivided into uniform cells. In this paper, a model is presented that is suitable for all frequency regimes of interest, and thus is most appropriate for transient interconnect analysis using a full-wave model denoted as (Lp, P, Z/sub s/, /spl tau/)PEEC, to indicate the inclusion of the complex skin effect model Z/sub s/.

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What this paper is about

A convenient skin effect model for the partial element equivalent circuits (PEEC) technique is the so-called volume filament technique. This approach is an integral part of the basic PEEC model if the conductor cross-sections are subdivided into cells. This model is efficient for geometries and frequencies where the skin depth is moderate compared to the conductor thickness. However, the computational cost may be too high for the case where the skin depth is a small fraction of the cross-section, especially if it is subdivided into uniform cells. In this paper, a model is presented that is suitable for all frequency regimes of interest, and thus is most appropriate for transient interconnect analysis using a full-wave model denoted as (Lp, P, Z/sub s/, /spl tau/)PEEC, to indicate the inclusion of the complex skin effect model Z/sub s/.

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Available abstract

A convenient skin effect model for the partial element equivalent circuits (PEEC) technique is the so-called volume filament technique. This approach is an integral part of the basic PEEC model if the conductor cross-sections are subdivided into cells. This model is efficient for geometries and frequencies where the skin depth is moderate compared to the conductor thickness. However, the computational cost may be too high for the case where the skin depth is a small fraction of the cross-section, especially if it is subdivided into uniform cells. In this paper, a model is presented that is suitable for all frequency regimes of interest, and thus is most appropriate for transient interconnect analysis using a full-wave model denoted as (Lp, P, Z/sub s/, /spl tau/)PEEC, to indicate the inclusion of the complex skin effect model Z/sub s/.

Key concepts: Partial element equivalent circuit, Skin effect, Conductor, Equivalent circuit, Interconnection, Physics, Electronic engineering, Computer science

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