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Overview of magnetic susceptibilities

The popular experimental techniques involve Faraday or Gouy balance measurements where the quantity being measured is the force acting on a body when it is in the magnetic field [Pg.114]

The work done in bringing the body of volume V with a uniform magnetisation M into a magnetic field is [Pg.114]

For isotropic non-ferromagnetic materials with volume susceptibility x it is d M = /d// [Pg.115]

When the sample is allowed to move in one direction (z) only, then one gets [Pg.115]

Evidently, the susceptibility subduced from such experiments is the mean mass susceptibility. This quantity, for linear magnetics, is close to the isothermal susceptibility. However, deviations from linear behaviour increase with [Pg.116]


See other pages where Overview of magnetic susceptibilities is mentioned: [Pg.114]    [Pg.115]   


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