Magnetization

Definition and stakes

Portrait of James Clerk Maxwell James Clerk Maxwell,  A Treatise on Electricity and Magnetism (1873)

“ In all substances except iron, nickel, and cobalt, the coefficient of magnetization is so small that the induced magnetization of the body produces only a very slight alteration of the forces in the magnetic field. We may therefore assume, as a first approximation, that the actual magnetic force within the body is the same as if the body had not been there. The superficial magnetization of the body is therefore, as a first approximation, , where is the rate of increase of the magnetic potential due to the external magnet along a normal to the surface drawn inwards. ”
Source: Wikisource

Shelford Bidwell,  1911 Encyclopædia Britannica, Volume 17… (1911)

“ If we twist the free end of a ferromagnetic wire while a current is passing through it, the wire becomes longitudinally magnetized, the direction of the magnetization depending upon circumstances: if the wire is of iron and is twisted so that its free end as seen from the fixed end turns in the direction of the hands of a watch, while the current passes from the fixed to the free end, then the direction of the resulting magnetization will be such as to make the free end a north pole. ”
Source: Wikisource

Shelford Bidwell,  1911 Encyclopædia Britannica, Volume 17… (1911)

“ The force in the interior is uniform, opposite to the direction of magnetization, and equal to 4/3πI. When it is desired to have a uniform magnet with definitely situated poles, it it usual to employ one having the form of an ovoid, or elongated ellipsoid of revolution, instead of a rectangular or cylindrical bar. If the magnetization is parallel to the major axis, and the lengths of the major and minor axes are 2a and 2c, the poles are situated at a distance equal to 2/3a from the centre, and the magnet will behave externally like a simple solenoid of length 4/3a. ”
Source: Wikisource

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