We learned about magnetic circuits in an earlier article and know from there that a current carrying conductor is surrounded by magnetic flux. Now suppose another conductor is placed in that magnetic field, what will happen? When the current in the first conductor changes it causes a corresponding variation in the associated magnetic flux, which will result in an induced emf in the secondary circuit.
This forms the basis of definition of mutual inductance which is defined as the phenomenon of emf being generated in one circuit when the current in the coupled circuit is varying. The formula which governs the generated emf is known as Faraday’s Law and it states that the emf induced in a circuit is directly proportional to the rate of change of magnetic flux through the circuit with time. Mathematically this law is expressed as
EMF = -N ∆BA/∆t
Where BA (B is the magnetic field, A is the area of the coil) stands for magnetic flux and t is time while N is the number of turns of the conductor. The negative sign denotes that the direction of the generated emf is such that the current generated tries to oppose the magnetic field producing it. This may seem quite paradoxical in that the current is trying to oppose the very source of its origin but it is known as Lenz’s law.
I also suggest that you take a good look at the diagram in figure 1 below as it beautifully depicts the phenomenon of mutual inductance in a pictorial format. As you can see from the picture, there are two independent circuits and when voltage is withdrawn from the circuit on the left hand side, it causes an emf in the right hand side circuits which tries to oppose that change.