In a paramagnetic material the magnetization of the material is (approximately) directly proportional to an applied magnetic field. However, if the material is heated, this proportionality is reduced; for a fixed value of the field, the magnetization is (approximately) inversely proportional to temperature. This fact is encapsulated by **Curie’s law**:

where

- is the resulting magnetisation
- is the magnetic field, measured in teslas
- is absolute temperature, measured in kelvins
- is a material-specific Curie constant.

This relation was discovered experimentally (by fitting the results to a correctly guessed model) by **Pierre Curie**. It only holds for high temperatures, or weak magnetic fields. As the derivations below show, the magnetization saturates in the opposite limit of low temperatures, or strong fields.

The **Curie–Weiss law** describes the magnetic susceptibility `χ` of a ferromagnet in the paramagnetic region above the Curie point:

where `C` is a material-specific Curie constant, `T` is absolute temperature, measured in kelvins, and `T _{c}` is the

*Curie temperature*, measured in kelvin. The law predicts a singularity in the susceptibility at

`T = T`. Below this temperature the ferromagnet has a spontaneous magnetization.

_{c}The magnetic moment of a magnet is a quantity that determines the torque it will experience in an external magnetic field. A loop of electric current, a bar magnet, an electron, a molecule, and a planet all have magnetic moments.

The **magnetization or magnetic polarization** of a magnetic material is the vector field that expresses the density of permanent or induced magnetic moments. The magnetic moments can originate from microscopic electric currents caused by the motion of electrons in individual atoms, or the spin of the electrons or the nuclei.

Net magnetization results from the response of a material to an external magnetic field, together with any unbalanced magnetic moment that may be present even in the absence of the external magnetic field; for example, in sufficiently cold iron. We call the latter spontaneous magnetization. Other materials that share this property with iron, like Nickel and magnetite, are called ferromagnets. The threshold temperature below which a material is ferromagnetic is called the Curie temperature and varies between materials.

## Limitation of Curie-Weiss Law

In many materials the Curie–Weiss law fails to describe the susceptibility in the immediate vicinity of the Curie point, since it is based on a mean-field approximation. Instead, there is acritical behavior of the form

with the critical exponent `γ`. However, at temperatures `T ≫ T _{c}` the expression of the Curie–Weiss law still holds, but with

`T`replaced by a temperature

_{c}`Θ`that is somewhat higher than the actual Curie temperature. Some authors call

`Θ`the

**Weiss constant**to distinguish it from the temperature of the actual Curie point.

# Curie Constant

The **Curie constant** is a material-dependent property that relates a material’s magnetic susceptibility to its temperature.

The Curie constant, when expressed in SI units, is given by

where

is the number of magnetic atoms (or molecules) per unit volume,

is the Landé g-factor,

(9.27400915e-24 J/T or A·m^{2}) is the Bohr magneton,

is the angular momentumquantum number and

is Boltzmann’s constant. For a two-level system with magnetic moment , the formula reduces to

The constant is used in **Curie’s Law**, which states that for a fixed value of a magnetic field, the magnetization of a material is (approximately) inversely proportional to temperature.

This equation was first derived by Pierre Curie.

Because of the relationship between magnetic susceptibility , magnetization and applied magnetic field :

this shows that for a paramagnetic system of non-interacting magnetic moments, magnetization .

##### Curie Weis Law Video Explaination – Curie’s Law and Curie – Weiss Law

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