Dynamic magnetization models for soft ferromagnetic materials with coarse and fine domain structures

被引:43
|
作者
Zirka, S. E. [1 ]
Moroz, Y. I. [1 ]
Steentjes, S. [2 ]
Hameyer, K. [2 ]
Chwastek, K. [3 ]
Zurek, S. [4 ]
Harrison, R. G. [5 ]
机构
[1] Dnepropetrovsk Natl Univ, Dept Phys & Technol, UA-49050 Dnepropetrovsk, Ukraine
[2] Rhein Westfal TH Aachen, Inst Elect Machines, D-52056 Aachen, Germany
[3] Czestochowa Tech Univ, Fac Elect Engn, PL-42201 Czestochowa, Poland
[4] Megger Instruments Ltd, Dover CT17 9EN, Kent, England
[5] Carleton Univ, Dept Elect, Ottawa, ON K1S 5B6, Canada
基金
加拿大自然科学与工程研究理事会;
关键词
Soft ferromagnetic materials; Magnetic losses; Loss separation; EDDY-CURRENT LOSS; NONORIENTED ELECTRICAL STEELS; POWER LOSSES; LOSS SEPARATION; IRON LOSSES; FREQUENCY; HYSTERESIS; LAMINATIONS; TRANSIENT; VOLTAGE;
D O I
10.1016/j.jmmm.2015.06.082
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We consider dynamic models, both numerical and analytical, that reproduce the magnetization field H(B) and the energy loss in ferromagnetic sheet materials with different domain structures. Conventional non oriented (NO) and grain oriented (GO) electrical steels are chosen as typical representatives of line domain and coarse domain materials. The commonly accepted loss separation procedures in these materials are critically analyzed. The use of a well-known simplified ("classical") expression for the eddy current loss is identified as the primary source of mistaken evaluations of excess loss in NO steel, in which the loss components can only be evaluated using the Maxwell (penetration) equation. The situation is quite different in GO steel, in which the loss separation is uncertain, but the total dynamic loss is several times higher than that explained by any version (numerical or analytical) of the classical approach. To illustrate the uncertainty of the loss separation in GO steel, we show that the magnetization field, and thus the total loss, in this material can be represented with equal accuracy using either the existing three-component approach or our proposed two-component technique, which makes no distinction between classical eddy-current and excess fields and losses. (C) 2015 Elsevier B.V. All tights reserved.
引用
收藏
页码:229 / 236
页数:8
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