As we saw above,
such a motor will work with a.c., although rather inefficiently. The motor will be a high-speed
motor whose speed is rather variable if the load is changed.
The shunt-wound motor cannot
he used in this way, since self-inductive effects in the field coils would result in the peaks of the
field in the armature and field coils getting out of phase, and so very little torque would be
obtained.
Such a motor has a single armature coil but three sets of field
coils, as shown in Figure 1.
The peaks of the current in each field coil occur at
different times and so the torque on the armature is fairly constant. If the rotor can be made to
rotate at the same rate as the field, it will be locked on to it and rotate at a constant speed with
the field.
This type of motor uses a set of three field coils, as in the
synchronous motor, but the rotor is of entirely different construction. It is made of a set of copper
bars fixed to two copper rings as shown in Figure 2, an arrangement known as a squirrel cage.
The rotating magnetic field in the field coils induces currents within these bars and the interaction
between these eddy currents and the field in the coils makes the rotor rotate.
Very
high speeds may be achieved and these motors have been used to propel shuttles on textile
looms, as aircraft launchers, to move conveyor belts and at low speed even to open and close
curtains!
In the shaded pole motor (Figure 3) a thick plate is fixed to the pole piece so that part of the surface of the pole piece is covered. Eddy currents are induced in this plate so producing another magnetic field. There is a phase difference between this field and the field in the pole. The aluminum disc sees these two out of phase fields as a moving field; eddy currents are induced in the disc which then rotates.