Liquids that are freely magnetised by magnetic fields are called diamagnetic liquids. In this case, magnetisation occurs in the opposite direction to the magnetic field. Diamagnetism is displayed in these materials.
Diamagnetic liquids are repellent to the external magnetic field. The orbital angular momentum of electrons in an atom is determined by their rotation around the nucleus. In the case of a diamagnetic material, the atom’s magnetic moment is nil.
According to Lenz’s law, when dipoles are induced in diamagnetic materials by an external magnetic field, the induced dipoles oppose the external field.
Diamagnetic liquids placed between two close pole pieces of glass create depressions in the centre, where the field is greatest, and liquid collects on the sides. When a liquid is poured over a watch glass between pole pieces that are sufficiently spaced apart (more than in the previous example), liquid collects in the centre, where the field is weakest. Due to the repulsion property, diamagnetic liquids in a U- tube depress in the arm placed between two poles of a magnet.
Water is one of the best-known examples of diamagnetic liquids. The mixture of ethanol and water shows good diamagnetic properties in the magnetisation curve.
In 1778, Anton Brugmans realised that magnetic fields repelled bismuth, which led to the discovery of diamagnetism. Michael Faraday accepted this as a property of matter and concluded that every material could be affected by a magnetic field. Faraday first named the phenomenon diamagnetic, which later evolved into diamagnetism.
Diamagnetic levitation takes place when a diamagnetic material is brought close to a material that produces a magnetic field. Diamagnetic material will repel magnetic field-producing material. However, this repelling force is generally not strong enough to overcome the forces of gravity on the earth’s surface. To achieve diamagnetic levitation, diamagnetic and magnetic materials must combine in a way that overcomes the earth’s gravity.
Diamagnetic levitation can be achieved in the ways given below:
In the presence of 15 Tesla magnetic fields, a frog is levitated. Water molecules within the frog’s body are magnetic, which produces the levitation force. Diamagnetism is best demonstrated in this way.
In a magnetic field, a superconductor behaves like a perfect diamagnetic material and excludes the magnetic field, so all flux lines do not penetrate the region. Diamagnetic superconductors are generally materials with a volume susceptibility equal to 1 (dimensionless). Since they tend to expel all magnetic fields, they can be considered true diamagnets.
Whenever a permanent magnet is brought near a superconductor, the magnet produces a magnetic field opposite to that of the superconductor. The interior of a superconductor is free of magnetic fields as a result of its expulsion from a magnetic field applied to it. This is the Meissner effect, due to which superconductors behave as a perfect diamagnet.
We learnt that diamagnetic liquids repel magnetic fields to penetrate them. Furthermore, they induce an opposite magnetic field, which is repulsive. The material reacts weakly to the external magnetic field, so it tends to move from a strong region to a weak region in a non-uniform field.
Materials with paired electrons, therefore, display diamagnetic properties. The magnetic moment of the atoms in diamagnetic substances is nil because of the paired electrons in the atoms. Diamagnetic substances are repelled by magnets.