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Zeeman energy : ウィキペディア英語版
Zeeman energy
Zeeman energy, or the external field energy, is the potential energy of a magnetised body in an external magnetic field. It is named after the Dutch physicist Pieter Zeeman, primarily known by the Zeeman effect. In SI units, it is given by
:E_ =-\mu_ \int_V\,\textbf M\cdot \textbf H_ \, \mathrm dV
where HExt is the external field, M the local magnetisation, and the integral is done over the volume of the body. This is the statistical average (over a
unit volume macroscopic sample) of a corresponding microscopic Hamiltonial (energy) for each individual magnetic moment m, which is however experiencing a ''local'' induction B:
:H =-\textbf m \cdot \textbf B
== References ==

* d'Aquino, M, Phd thesis, http://wpage.unina.it/mdaquino/PhD_thesis/main/node16.html
* Hubert, A. and Schäfer, R. Magnetic domains: the analysis of magnetic microstructures, Springer-Verlag, 1998

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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