# Shaded Pole Induction Motor - Construction, Working Principle & Applications

As we know that a single-phase induction motor is not a self-starting motor. In order to make it self starting, changes are to be done to the construction. Let us see the construction and working principle of the shaded pole induction motor.

## Construction of Shaded Pole Induction Motor :

The construction of a shaded type induction motor is similar to a normal single-phase induction motor, except for its stator pole. The stator poles of a shaded pole motor are divided into two parts.

One part of the pole consists of a short-circuited coil made up of copper which is known as the shading coil (shaded part) and the remaining part is known as the unshaded part of the pole, hence the motor is known as a shaded pole induction motor.

The construction of the rotor is of a normal squirrel cage type of a 3-phase induction motor. The below figure shows the single-phase two-pole induction motor with a shading coil on both the stator poles. Check out this animated video for more detailed explanations.

## Working Principle of Shaded Pole Induction Motor :

When a single-phase a.c. supply is given to the stator winding. The poles of the motor generate a magnetic field Φm, but there is one more magnetic field Φs produced by shading coils either in the same or opposite direction.

The combination of these fields makes a rotating magnetic field which makes the rotor rotate. Let us consider three different cases at different time instants t1, t2, and t3 on a positive half cycle of an ac supply.

### Case-1 (At instant t = t1) :

As seen from the waveform, at instant t = t1. The current in the coil increases, which in turn increases the flux Φm produced by the coil. Now due to supply is alternating, the rate of change of flux will tends to cause an emf induced in a shading coil of that pole.

As the shading coil is short-circuited, currents will flow through it. Simultaneously causes to produces another flux Φs by the shading coil, which in the opposite direction to the main flux as shown below.

Now due to the opposition of these two fluxes produced by the shading coil and main winding. The net flux across the area of the shading coil will be zero. Therefore, the magnetic axis of the net flux will be at the center of the unshaded part.

### Case-2 (At instant t = t2) :

Now, at instant t = t2 i.e., the maximum or peak value of the cycle or current. Here further there will be no increase in the current (no change of current). So it decreases the rate of change of flux, which also decreases the emf induced in the shading coil. At this point, the flux Φs produced by the shading coil will be almost negligible.

Hence the flux Φm produced by the main winding will be uniformly distributed along the pole. Therefore, the magnetic axis of the pole will be at the center of the whole pole (with shaded and unshaded parts) as shown below.

### Case-3 (At instant t = t3) :

At this instant, the rate of change of current will be in decreasing. As the current changes, there will be an induced emf in the shading coil due to the change of flux.

But here the direction of the fluxes Φm and Φs produced by both the main winding and shading coil will be in the same direction. Also there will be crowding of flux in the shaded part as compared to the unshaded part. Due to this, the net magnetic axis of the pole will be at the center of the shading part of that pole, as shown below.

This sequence of instants keeps on repeating for the negative half cycle also. As it will result in the production of a rotating magnetic field. By which the motor tends to start on its own. The starting torque produced by this type of motor will be 50% to 60% of the full-load torque.