Abstract

For magnetic energy loss measurements on electric steel sheets, the Epstein tester (ET) is applied for 100 years. However, it suffers from unsolved problems, such as inhomogeneity of flux in the corners and even more of impact of sample cutting. As a matter of fact, a detailed study of flux distributions—as a pre-condition for improvements—has not been performed so far. In this work, we present the results of an advanced numerical 3D-magnetic anisotropic circuit calculation modeling. It considers most relevant impacts such as anisotropy, non-linearity, method of staggering, and in particular, consequences of sample cutting. According to the literature, the latter may yield material deterioration for edge zones of high width WDET. Here, we set WDET to 2.5 mm as a “coarse-cut” convention for practice, and we compare it with perfect “fine-cut” (W = 0). As a main result, deteriorated edge zones of standard ET strips of low width W = 30 mm yield a distinct concentration of flux along inner axial strip regions as a reason for strong local flux inhomogeneity and distortion. Consistent numerical comparisons predict that higher grades of magnetic homogeneity can be expected from wider sample strips, e.g., from a “Triple ET” with W = 90 mm. As a global conclusion, the Epstein frame represents a system of extreme 3D inhomogeneity, especially in the corners. The grade of inhomogeneity reaches its maximum in instants of high permeability. It may be strongly increased through coarse cutting. On the other hand, consequences of cutting can be decreased by increasing the strip width. This would allow for loss measurements using tangential field coils arranged in the central limb regions of TET.

Highlights

  • Worldwide attempts are made to increase the effectiveness of electric machines that exhibit soft-magnetic cores, as manufactured from silicon iron laminations

  • This yields demands for the exact knowledge on magnetic energy losses P of different types of electric steel

  • (2) The usual assessment of Epstein tester (ET) for instants of peak induction BPEAK is ineffective because of promising homogeneity due to low permeability μ, apart from zero instantaneous loss p. (3) Effective assessments are possible for instantaneous B around 1 T due to high values of both μ and p. (4) The corresponding inhomogeneity of ET is strongly underestimated so far, depending on the anisotropy of the material

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Summary

INTRODUCTION

Worldwide attempts are made to increase the effectiveness of electric machines that exhibit soft-magnetic cores, as manufactured from silicon iron laminations. This yields demands for the exact knowledge on magnetic energy losses P of different types of electric steel. The additional standard concerns the Epstein frame, in the following referred to as Standard Epstein Tester (SET). It is much more compact than the SST, but it suffers from a physically much less convincing principle. We report results of an advanced corresponding numerical study of modeling

PRE-CONDITIONS
PROCEDURE OF MACC MODELING OF EPSTEIN FRAME
STANDARD EPSTEIN TESTER WITH FINE-CUT SAMPLE STRIPS
STANDARD TESTER WITH COARSE-CUT SAMPLE STRIPS
Coarse-cut NO steel
Coarse-cut GO steel
Conclusions for standard Epstein tester
TRIPLE EPSTEIN TESTER WITH FINE-CUT SAMPLE STRIPS
TRIPLE EPSTEIN TESTER WITH COARSE-CUT SAMPLE STRIPS
VIII. DISCUSSION
Findings
CONCLUSIONS
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