The individual atoms (or ions or molecules) of a paramagnetic material possess a permanent magnetic dipole moment of their own. On account of the ceaseless random thermal motion of the atoms, no net magnetisation is seen. In the presence of an external field B0, which is strong enough, and at low temperatures, the individual atomic dipole moment can be made to align and point in the same direction as B0. Figure shows a bar of paramagnetic material placed in an external field. The field lines gets concentrated inside the material, and the field inside is enhanced. In most cases, this enhancement is slight, being one part in 105. When placed in a non-uniform magnetic field, the bar will tend to move from weak field to strong.
Example : Some paramagnetic materials are aluminium, sodium, calcium, oxygen (at STP) and copper chloride.
Experimentally, one finds that the magnetisation of a paramagnetic material is inversely proportional to the absolute temperature T,
or equivalently,
This is known as Curie law, after its discoverer Pieree Curie (1859- 1906). The constant C is called Curie constant. Thus, for a paramagnetic material both χ and μr depend not only on the material, but also (in a simple fashion) on the sample temperature. As the field is increased or the temperature is lowered, the magnetisation increases until it reaches the saturation value MS, at which point all the dipoles are perfectly aligned with the field. Beyond this, Curie longer valid.
