Analytical optimization of litz-wire windings independent of porosity factor

Author:

Wojda Rafal P.,Kazimierczuk Marian K.

Abstract

Purpose – The purpose of this paper is threefold. First, an analytical model based on one-dimensional Dowell’s equation for computing ac-to-dc winding resistance ratio FR of litz wire is presented. The model takes into account proximity effect within the bundle and between bundle layers as well as the skin effect. Second, low- and medium-frequency approximation of Dowell’s equation for the litz-wire winding is derived. Third, a derivation of an analytical equation is given for the optimum strand diameter of the litz-wire winding independent on the porosity factor. Design/methodology/approach – The methodology is as follows. First, the model of the litz-wire bundle is assumed to be a square shape. Than the effective number of layers in the litz wire bundle is derived. Second, the litz-wire winding is presented and an analytical equation for the winding resistance is derived. Third, analytical optimization of the strand diameter in the litz-wire winding is independent on the porosity factor performed, where the strand diameter is independent on the porosity factor. The boundary frequency between the low-frequency and the medium-frequency ranges for both solid-round-wire and litz-wire windings are derived. Hence, useful frequency range of both windings can be determined and compared. Findings – Closed form analytical equations for the optimum strand diameter independent of the porosity factor are derived. It has been shown that the ac-to-dc winding resistance ratio of the litz-wire winding for the optimum strand diameter is equal to 1.5. Moreover, it has been shown that litz-wire winding is better than the solid-round-wire winding only in specific frequency range. At very high frequencies the litz-wire winding ac resistance becomes much greater than the solid-round-wire winding due to proximity effect between the strands in the litz-wire bundle. The accuracy of the derived equations is experimentally verified. Research limitations/implications – Derived equations takes into account the losses due to induced eddy-currents caused by the applied current. Equations does not take into account the losses caused by the fringing flux, curvature, edge and end winding effects. Originality/value – This paper presents derivations of the closed-form analytical equations for the optimum bare strand diameter of the litz-wire winding independent on the porosity factor. Significant advantage of derived equations is their simplicity and easy to use for the inductor designers.

Publisher

Emerald

Subject

Applied Mathematics,Electrical and Electronic Engineering,Computational Theory and Mathematics,Computer Science Applications

Reference40 articles.

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2. Bartoli, M. , Noferi, N. , Reatti, A. and Kazimierczuk, M.K. (1995), “Modeling winding losses in high-frequency power inductors”, Journal of Circuits, Systems and Computers Vol. 5 No. 4, pp. 607-626.

3. Bartoli, M. , Reatti, A. and Kazimierczuk, M.K. (1996), “Minimum copper and core losses power inductors design”, Proceedings of the 1996 Thirty-First IEEE Industry Applications Society IAS Annual Meeting, 6-10 October, San Diego, CA.

4. Dowell, P.J. (1966), “Effects of eddy currents in transformer winding”, Proc. IEE , Vol. 113 No. 8, pp. 1387-1394.

5. Field, A.B. (1905), “Eddy currents in large slot-wound conductors”, Transactions of the American Institute of Electrical Engineers , Vol. 88, pp. 1125-1143.

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