Above a critical temperature* T _{c}*, the Curie temperature,
all ferromagnetic materials become paramagnetic. This is because thermal energy
is large enough to overcome the cooperative ordering of the magnetic moments.

The susceptibility of a material, χ, indicates how dramatically a material
responds to an applied magnetic field, and is defined as the ratio of the magnetisation
of the material, *M*, and the applied magnetic field,* H*.

\[\chi = \frac{M}{H}\;\;\;\;{\rm{equation}}\;1\]

The magnetisation of a material, *M*, is defined as the magnetic moment
per unit volume or per unit mass of a material and is dependent on the individual
magnetic dipole moments of the atoms in the material and on the interactions
of these dipoles with each other.

Above the Curie Temperature there will be a change in the susceptibility as the material becomes paramagnetic, therefore giving the equation:

\[\chi = \frac{C}{{T - {T_c}}} = \frac{M}{H}\;\,\,\,{\rm{equation}}\;2\]

where *C* is a constant.

The graph below shows the saturation magnetisation (ie that obtained in a high magnetic field) of a ferromagnetic element, nickel, as a function of temperature. We see that the saturation magnetisation decreases with increasing temperature until it falls to zero at the Curie temperature where the material becomes paramagnetic:

Differentiation of Equation 2 with respect to temperature shows that the susceptibility is a maximum at the Curie temperature. This is no surprise; it is easiest to increase the magnetic moment of the material by applying a magnetic field when the material is undergoing a transition between magnetic order and disorder. The graph below for nickel shows the susceptibility tending to infinity as the temperature moves closer to the Curie temperature:

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