The magnetic forces of a material’s electrons will be changed when put in a magnetic field. Faraday’s law of magnetic induction describes this phenomenon. The magnetic properties determine how it responds to an external magnetic force.
Materials are classified into three types by their response to externally applied magnetic fields: diamagnetic, paramagnetic, or ferromagnetic fields. Atoms of materials that show diamagnetic behaviour have no permanent magnetic dipole moment.
When a diamagnetic material is introduced in an external magnetic field, a weak and slim magnetic dipole moment is induced in the direction of the applied field. Without applying a magnetic field, diamagnetic materials have no net magnetic moment (H). The spin motion of electrons and their interactions with one another are the origins of magnetism.
When diamagnetic material is subjected to an external magnetic field, the spinning electrons undergo a motion that produces an electrical current, resulting in magnetisation in the opposite direction of the magnetic field.
When an electron in an atomic orbit moves through a magnetic field, the force applied on the electron causes a slight shift in orbital motion; the electron orbit processes around the magnetic field’s direction. The properties of diamagnetic materials vary in nature.
The magnetic properties possessed by the atoms and ions of a material are responsible for the magnetic properties shown by the material. The revolution of the atoms around the nucleus of the atom and the spin of the electrons in their axis causes the magnetic properties of the materials. Materials are classified into five types depending on their magnetic properties. They include:
The orbital motion of electrons produces magnetic fields by creating atomic current loops. When a material that shows the diamagnetic property is subjected to an external magnetic field, the current spins will tend to arrange themselves to act opposite to the applied field.
In diamagnetism, electrons inside a material respond to an external magnetic field by rotating rapidly, creating magnetic forces opposing the external field. All materials are diamagnetic to some degree since all atoms contain electrons. However, if diamagnetism is present, the greater forces of paramagnetism or ferromagnetism will quickly outnumber it. All these are together responsible for the different properties of diamagnetism.
When a substance is put in an external magnetic field, its susceptibility measures how much it becomes magnetised.
The magnetic susceptibility of a material is denoted by the Greek letter chi (χ).
It is expressed as the magnitude of the internal polarisation (J) divided by the strength of the external field (B0):
χ = J / B0
Diamagnetic materials resist the magnetic field; hence magnetic susceptibility is negative for diamagnetic materials. The spin in a diamagnetic substance is aligned in the opposite direction of the applied magnetic field. The value of susceptibility is not dependent on temperature.
The capacity of diamagnetic materials to reject force lines is known as permeability (due to the structure of diamagnetic material). They reject force lines and prevent magnetic lines of force from passing through them. As a result, the 1 for diamagnetic materials.
The ratio of internal magnetisation to the applied magnetic field is measured by magnetic permeability.
When diamagnetic material is placed in a magnetic field, the magnetic force lines prefer not to pass through it as if the diamagnetic substance was ejecting magnetic field lines. As a result, the sample’s magnetic field lines reduce to a lesser value.
Magnetic fields have a weak and negative susceptibility in diamagnetic materials. When a magnetic field is applied, diamagnetic materials are somewhat repelled and lose their magnetic qualities when the field is withdrawn. Diamagnetic materials are made up of atoms with no net magnetic moments. Only if there are no other magnetic effects present, such as ferrimagnetism, whose susceptibility is substantially higher in most circumstances, does a material’s diamagnetic response contribute to its magnetisation. Diamagnetism exists in all materials. It is temperature independent and is often disregarded since it is so little compared to ferromagnetic and paramagnetism effects.