scholarly journals A Magnetic Phenomena Analysis by Employing Particle Method and Magnetic Moment Method

Author(s):  
Kenta Mitsufuji ◽  
Katsuhiro Hirata ◽  
Fumikazu Miyasaka ◽  
Shuhei Matsuzawa
2016 ◽  
Vol 5 (4) ◽  
pp. 355-359 ◽  
Author(s):  
Kenta Mitsufuji ◽  
Shuhei Matsuzawa ◽  
Katsuhiro Hirata ◽  
Fumikazu Miyasaka

2013 ◽  
Vol 423-426 ◽  
pp. 2104-2107
Author(s):  
Tatyana N. Gnitetskaya ◽  
Elena V. Karnauhova

A qualitative proof of diamagnetic non-zero magnetization based on the electromagnetic induction law is presented in this paper. Modeling diamagnetic phenomena as a result of Larmor precession or effect of the electromagnetic induction’s law in scale of one hydrogen-like atom performed in classical physics contributes to formation of obviously incorrect idea of the diamagnetic magnetization process in students. It is well-known that the average magnetic moment of a diamagnetic calculated with the help of classical statistics laws is zero which can be explained by quantum character of magnetic phenomena. On the contrary, electromagnetic induction’s law is effective both in classical and quantum physics. Applying it to the diamagnetism problem will allow to solve it for the diamagnetic in whole and to avoid averaging which is proved in the present paper.


The accurate experiments of Chattock and Bates prove that the angular momentum arising in a ferromagnetic substance from unit change in its magnetic moment is very nearly, if not exactly, one half the value 2 m/e = 1.13 X 10 -7 , which seemed to me the most likely when I first discussed this effect. This conclusion is supported by the fact that the improvements which have been introduced into this subject by successive experimenters in recent years have led to values showing a strong tendency to settle at the same limit m/e = 5.65 X 10 -8 . This value is also in general agreement with that deduced by Barnett from experiments on the converse effect. It seems desirable therefore to reconsider the interpretation of this ratio. The higher value 2 m/e is obtained by making rather definite assumptions, which evidently require modification, as to the nature of the phenomena. These assumptions are that the process of magnetization involves the turning of electron orbits, and that nothing else which may occur has any important influence on the phenomena. The inertia of the electrons is assumed to be entirely of the type which controls the deflection of a beam of cathode rays by a magnetic field, and any change in the motion of the positively charged part of the atom is disregarded. These assumptions are essentially the same as those of the theories of Langevin and Weiss which have been successful in dealing with purely magnetic phenomena.


1968 ◽  
Vol 23 (12) ◽  
pp. 1911-1913
Author(s):  
Siegfried Hess

The influence of a magnetic field on the diffusion of Brownian particles with a magnetic moment parallel to their internal angular momentum is discussed. Starting point is a generalized Fokker-Planck equation. Application of the moment method leads to a set of transport-relaxation equations. From them the diffusion tensor depending on the external field is inferred.


2008 ◽  
Vol 44 (6) ◽  
pp. 1014-1017 ◽  
Author(s):  
H.L. Rakotoarison ◽  
V. Ardon ◽  
O. Chadebec ◽  
B. Delinchant ◽  
S. Guerin ◽  
...  

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