An electric current can be induced in a coil by flux change produced by another coil in its proximity or flux change produced by the same coil. In both cases, the flux through the coil is proportional to the current.
That is, ØB ∝ I
For a closely looped coil of N turns, the same magnetic flux is linked with all the turns. When the flux ∅B through the coil changes, each turn contributes to the generated electromotive force. This is described using the term flux linkage which is equal to N∅B for a closely wound coil. In such a case,
NØB ∝ I
The constant of proportionality in this context is called inductance. It is affected by the shape of the coil and core material properties. It is a scalar quantity.
Henry is the SI unit of inductance. It is denoted by H. It is named after Joseph Henry, an eminent physicist who discovered electromagnetic induction in the USA, independently of Faraday in England.
When an electric current is induced in a coil due to flux change in the coil’s proximity, it is called mutual inductance. In simple words, when a voltage change in one coil induces a voltage in another coil near it, it is known as mutual inductance. The formula for mutual inductance is as follows:
Here,
N1 = Turns of coil 1
N2 = Turns of coil 2
A = Cross-sectional area in m2
L= Length of the coil in metres
μ0 = Permeability of free space= 4𝜋*10-7
μr = Relative permeability of the soft iron core
The distance between the coils and the shape of the coils affects the mutual inductance of two coils, solenoids, etc.
N1∅1=M12I2
The functions of mutual inductance in physics are as follows:
Mutual-Inductance | Self-Inductance |
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Mutual inductance can be described as the electromotive force induced when one coil’s magnetic field opposes the change of voltage and current in another coil. The coils become magnetically linked due to changes in magnetic flux. Henry is the SI unit of inductance. It is denoted by H. When the primary current of the coil decreases, the induced current of the other coil opposes the decay of current in the coil. When the primary current of the coil increases, the induced current of the other coil opposes the increase of current in the coil. Examples are transformers, electric motors, generators, etc.