Affiliations: [a] Nanoscience and Materials Division, Istituto Nazionale di Ricerca Metrologica, Torino, Italy | [b] Energy Department, Politecnico di Torino, Torino, Italy | [c] SATIE-ENS, UniverSud, Cachan, France
Correspondence:
[*]
Corresponding author: Enzo Ferrara, Nanoscience and Materials Division, Istituto Nazionale di Ricerca Metrologica, Torino, Italy. E-mail: [email protected].
Abstract: The magnetic power losses have been measured at 50 Hz and different peak polarization values on different types of non-oriented and grain-oriented Fe-Si sheets using the Epstein frame, according to the current standards. The very same measurements have then been repeated by measuring polarization and tangential magnetic field by means of localized windings, centrally placed on the strips inside the Epstein frame windings, thereby retrieving the effective field and the true power loss figure. It is obtained that the ratio of the standard P๐๐๐ ๐ก to the effective P๐๐๐ loss figure, which can be interpreted in terms of ratio of effective l๐๐๐ to conventional (lm= 0.94ย m) magnetic path length, evolves with the peak polarization Jp, showing, in general, a monotonic increase with increasing Jp. The deviation of P๐๐๐ ๐ก from P๐๐๐ is observed to range from about -3% in the non-oriented alloys at low inductions to about +5% in the grain-oriented alloys at Jp= 1.8 T. This behavior finds a rationale in the existence of a polarization profile Jpโข(x) measured along the strip length and in the dependence of P๐๐๐ on Jp, showing a power law P๐๐๐โข(Jp)โJpn, with n>1 and increasing with Jp. The so calculated effective path length leโขfโขf=lmโ P๐๐๐ ๐ก/P๐๐๐ consistently shows a monotonic increase with Jp, which is more relevant in the GO alloys.
Keywords: Magnetic power losses, Epstein frame, magnetic steels
