2015
DOI: 10.1109/tmag.2014.2353691
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Anisotropic Generalization of Vector Preisach Hysteresis Models for Nonoriented Steels

Abstract: A Preisach-type vector hysteresis model is developed to represent anisotropic material characteristics under static and dynamic conditions. Bi-and uniaxial anisotropy are incorporated by generalizing the input projection of the vector model. Frequencydependent eddy current and excess effects are considered by an additional field strength component. The model is applied to simulate the magnetic properties of weakly anisotropic nonoriented magnetic steel. The simulation results are successfully validated against… Show more

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Cited by 26 publications
(14 citation statements)
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“…The hysteresis, both static and dynamic [24], [25], is deliberately omitted from the FEM simulations when they are concerned with condition monitoring. This is the case for the anisotropy characteristic of iron sheets too [26].…”
Section: B Finite Element Simulationsmentioning
confidence: 99%
“…The hysteresis, both static and dynamic [24], [25], is deliberately omitted from the FEM simulations when they are concerned with condition monitoring. This is the case for the anisotropy characteristic of iron sheets too [26].…”
Section: B Finite Element Simulationsmentioning
confidence: 99%
“…The BH measurement data used in this paper corresponds to 0.5 mm non-oriented (NO) silicon-iron electrical steel (grade M400-50A). The magnetic measurements are obtained from a rotational single-sheet tester (RSST) [16], [17]. The measurement is a B-controlled and performed at 50 Hz.…”
Section: Introductionmentioning
confidence: 99%
“…Among diverse methods for predicting locally the isotropic hysteresis, the mathematical Preisach model and the phenomenological Jiles-Atherton (J-A) model received a growing attention these last decades. In order to account for the anisotropic behaviour of electrical steel sheets, the improvement of the Preisach model can be performed either with a phenomenological bistroide model (Vernescu-Spornic et al, 2000) or with a generalized Mayergoyz model (Mayergoyz, 2003;Dlala, 2011;Handgruber et al, 2015). Although the former presents some discrepencies at low amplitude of the flux density under rotational field, the diverse improvements of the latter can accuratly represent both alternating and rotating dissipative behaviour, including the excess field, of the ferromagnetic materials.…”
Section: Introductionmentioning
confidence: 99%
“…The modification consists in replacing the Langevin anhysteretic curves by the interpolation of every components of the anhysteretic magnetization with respect to all the components of the effective field. Hence, only three diagonal tensors are identified from alternating flux density measurements at 50 Hz in principal directions (Goričan et al, 2000;Handgruber et al, 2015). The proposed improvement is then compared with both the anisotropic J-A model and the rotating flux density measurements.…”
Section: Introductionmentioning
confidence: 99%