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Materials with permanent atomic magnetic moments arranged in parallel in different domains are called ferromagnetic materials.
Without a magnetic field, the domains are randomly oriented. However, all the domains tend to orient along the field direction under an external magnetic field. Further, the size of the aligned domains increases at the expense of the unaligned ones. The combined processes result in substantial magnetization of the ferromagnet.
Under an external field, a ferromagnet's magnetization increases until it reaches magnetic saturation. Reducing the field to zero does not lead to zero magnetization. This property of ferromagnets to retain the magnetization is called hysteresis.
When the field is reversed, the domains slowly flip, and the magnetization reaches zero at the coercive field. The domain flipping continues untill the magnetization saturates.
Reducing the field to zero again leads to non-zero magnetization. The process continues as the field is reversed, and a complete hysteresis loop is obtained.
Ferromagnets have relative permeability much greater than unity. Thus, the susceptibility is positive and very high. Ferromagnets turn into paramagnets at Curie temperature.
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnet…
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