2006
DOI: 10.1109/tmag.2006.880090
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Measurement and Modeling of$B$–$H$Loops and Losses of High Silicon Nonoriented Steels

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Cited by 32 publications
(25 citation statements)
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“…4(a), dynamic loops predicted by the DHM-B are a good first approximation of those obtained experimentally (a method 22,23 of improving the DHM-B will be mentioned at the end of this section). On the contrary, the dynamic loops in Fig.…”
Section: Non-physical Behavior Of the Jiles Dynamic Hysteresis Mmentioning
confidence: 67%
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“…4(a), dynamic loops predicted by the DHM-B are a good first approximation of those obtained experimentally (a method 22,23 of improving the DHM-B will be mentioned at the end of this section). On the contrary, the dynamic loops in Fig.…”
Section: Non-physical Behavior Of the Jiles Dynamic Hysteresis Mmentioning
confidence: 67%
“…Under these conditions, the loss separation (8) is equivalent to the field separation 22,23 HðtÞ ¼ H hyst ðtÞ þ H clas ðtÞ þ H exc ðtÞ;…”
Section: Non-physical Behavior Of the Jiles Dynamic Hysteresis Mmentioning
confidence: 99%
“…The first material, Steel-0.1, is 0.1 mm thick, 5.5% Si, r ¼ 0.735 mO m, while the other, Steel-0.5, is 0.5 mm thick, 1.8% Si, r ¼ 0.432 mO m. It was shown in Ref. [8] that the TSM applied to high silicon Steel-0.1 provides the same accurate prediction of the dynamic loops and losses (up to 1 kHz and B m ¼ 1.3 T) as the MDM [1]. The measured loss dependence shown in Fig.…”
Section: Article In Pressmentioning
confidence: 88%
“…A convenient tool to include excess loss in the total loss evaluation is the thin sheet model (TSM) [8], which enables the total loss (W ¼ W h +W clas +W exc ) to be calculated as:…”
Section: Excess Loss Evaluationmentioning
confidence: 99%
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