Standardization of anhysteretic magnetization curves

2005 ◽  
Vol 97 (10) ◽  
pp. 10E504
Author(s):  
Jozef Kwiczala ◽  
Bogusław Kasperczyk

Theoretical anhysteretic magnetization curves are derived by searching for the minimum energy in an applied field of model domain structures. Magnetization curves are derived for: (1) Finite uniaxial crystals with 180° plane parallel walls. (2) Slightly misoriented polycrystals with (a) plane parallel walls, (b) walls allowed to bow. (3) Oriented polycrystalline materials with air gaps at the grain boundaries. The third model is found to be unrealistic, for a polycrystalline material without any second phase at the grain boundaries, and it is shown that the observed magnetization behaviour may be more generally accounted for in terms of the misorientation between grains. The calculations are precise, but the results are dependent on the initial choice of model domain structure and any limitations imposed on the way in which the walls move.


AIP Advances ◽  
2017 ◽  
Vol 7 (5) ◽  
pp. 056013 ◽  
Author(s):  
Simon Steentjes ◽  
Martin Petrun ◽  
Gregor Glehn ◽  
Drago Dolinar ◽  
Kay Hameyer

2012 ◽  
Vol 61 (4) ◽  
pp. 455-470 ◽  
Author(s):  
Krzysztof Chwastek

Abstract Some physical concepts important for a hysteresis model (effective field, anhysteretic magnetization) are discussed on the example of Jiles-Atherton model. The Jiles-Atherton model reveals some drawbacks, which make this model more difficult to be applied in electrical engineering. In particular, it does not describe accurately the magnetization curves after a reversal, moreover complex magnetization cycles are poorly represented. On the other hand, the phenomenological description proposed by Takács seems to be a valuable alternative to the Jiles-Atherton formalism. The concept of effective field may be easily incorporated in the description.


2017 ◽  
Vol 68 (3) ◽  
pp. 478-482 ◽  
Author(s):  
Katarzyna Bloch

This paper presents the results of numerical analysis of the primary magnetization curves, which were obtained under the assumptions of the theory of approach to ferromagnetic saturation described in by H. Kronm�ller. Test samples of the Fe78Si11B11 alloy were tape-shaped materials, which were subjected to isothermal annealing, not causing their crystallization. The investigated ribbons (tapes) were characterized by a very high saturation magnetization value of approximately 2T, which the thermal treatment has increased by about 10%. It was found that reason for the change of saturation magnetization of the investigated samples was the local rearrangement of atoms due to diffusion processes leading to the release of free volumes to the surface and combining of them into larger unstable defects called pseudodislocational dipoles.


1996 ◽  
Vol 263 (1-4) ◽  
pp. 442-445 ◽  
Author(s):  
T. Noji ◽  
T. Takabayashi ◽  
T. Nishizaki ◽  
N. Kobayashi ◽  
Y. Koike

1993 ◽  
Vol 200 (1-4) ◽  
pp. 413-419 ◽  
Author(s):  
L. Klein ◽  
E.R. Yacoby ◽  
Y. Yeshurun ◽  
M. Konczykowski ◽  
K. Kishio

2013 ◽  
Vol 818 ◽  
pp. 72-76 ◽  
Author(s):  
Gang Su

The crystalline electric field parameters Anmfor HoFe11Ti under different pressures were evaluated by fitting calculations to the magnetization curves measured on the single crystals at several temperatures. It was found that magneto-crystalline anisotropy has been changed by high pressure and the Anmfor HoFe11Ti under high pressures are strikingly different from Anmfor the corresponding HoFe11Ti H with interstitial hydrogen atom.


Sign in / Sign up

Export Citation Format

Share Document