The invention of induction motors permanently altered the course of human civilization. This hundred-year-old motor—invented by the great scientist Nikola Tesla—is the most common motor type, even today. In fact, about 50 percent of global electric power consumption is due to induction motors. Let’s get into the workings of induction motors, or more specifically, into Nikola Tesla’s genius thinking.
A detailed webpage version of the video is given below.
An induction motor has 2 main parts; the Stator and Rotor (Fig:1). The Stator is the stationary part and the rotor is the rotating part. The stator is basically a 3 coil winding and three phase AC power input is given to it. The Rotor sits inside the Stator. There will be a small gap between rotor and stator, known as air-gap. The value of the radial air-gap may vary from 0.5 to 2 mm.
A Stator is made by stacking thin-slotted highly permeable steel laminations inside a steel or cast iron frame. The way the steel laminations are arranged inside the frame is shown in the following figure. Here only few of the steel laminations are shown. Winding passes through slots of the stator.
When a 3 phase AC current passes through the winding something very interesting happens. It produces a rotating magnetic field (RMF). As shown in the figure below a magnetic field is produced which is rotating in nature. RMF is an important concept in electrical machines. We will see how this is produced in the next section.
To understand the phenomenon of a rotating magnetic field, it is much better to consider a simplified 3 phase winding with just 3 coils. A wire carrying current produces a magnetic field around it. Now for this special arrangement, the magnetic field produced by 3 phase A.C current will be as shown at a particular instant.
The components of A.C current will vary with time. Two more instances are shown in the following figure, where due to the variation in the A.C current, the magnetic field also varies. It is clear that the magnetic field just takes a different orientation, but its magnitude remains the same. From these 3 positions it’s clear that it is like a magnetic field of uniform strength rotating. The speed of rotation of the magnetic field is known as synchronous speed.
Assume you are putting a closed conductor inside such a rotating magnetic field. Since the magnetic field is fluctuating an E.M.F will be induced in the loop according to Faraday’s law. The E.M.F will produce a current through the loop. So the situation has become as if a current carrying loop is situated in a magnetic field. This will produce a magnetic force in the loop according to Lorentz law, So the loop will start to rotate, this is clearly illustrated in Fig:6.
A similar phenomenon also happens inside an induction motor. Here instead of a simple loop, something very similar to a squirrel cage is used. A squirrel cage has got bars which are shorted by end rings.
A 3 phase AC current passing through a Stator winding produces a rotating magnetic field. So as in the previous case, current will be induced in the bars of the squirrel cage and it will start to rotate. You can note variation of the induced current in squirrel cage bars. This is due to the rate of change of magnetic flux in one squirrel bar pair which is different from another, due to its different orientation. This variation of current in the bar will change over time.
That’s why the name induction motor is used, electricity is induced in rotor by magnetic induction rather than direct electric connection. To aid such electromagnetic induction, insulated iron core lamina are packed inside the rotor.
Such small slices of iron layers make sure that eddy current losses are at a minimum. You can note one big advantage of 3 phase induction motors, as it is inherently self starting.
You can also note that the bars of a squirrel cage are inclined to the axis of rotation, or it has got a skew. This is to prevent torque fluctuation. If the bars were straight there would have been a small time gap for the torque in the rotor bar pair to get transferred to the next pair. This will cause torque fluctuation and vibration in the rotor. By providing a skew in the rotor bars, before the torque in one bar pair dies out, the next pair comes into action. Thus it avoids torque fluctuation.
You can notice here that the both the magnetic field and rotor are rotating. But at what speed will the rotor rotate?. To obtain an answer for this let’s consider different cases.
Consider a case where the rotor speed is same as the magnetic field speed. The rotor experiences a magnetic field in a relative reference frame. Since both the magnetic field and the rotor are rotating at same speed, relative to the rotor, the magnetic field is stationary. The rotor will experience a constant magnetic field, so there won’t be any induced e.m.f and current. This means zero force on the rotor bars, so the rotor will gradually slow down. But as it slows down, the rotor loops will experience a varying magnetic field, so induced current and force will rise again and the rotor will speed up. In short, the rotor will never be able to catch up with the speed of the magnetic field. It rotates at a specific speed which is slightly less than synchronous speed. The difference in synchronous and rotor speed is known as slip.
The rotational mechanical power obtained from the rotor is transferred through a power shaft. In short in an induction motor, electrical energy is enters via the Stator and output from the motor,the mechanical rotation is received from the rotor.
But between the power input and output, there will be numerous energy losses associated with the motor. Various components of these losses are friction loss, copper loss, eddy current and hysteresis loss. Such energy loss during the motor operation is dissipated as heat, so a fan at the other end helps in cooling down the motor.
Now, let’s understand why induction motors rule both the industrial and domestic worlds. You can note that induction motors do not require a permanent magnet. They do not even have brushes, commutator rings or position sensor like other electrical machine counterparts. Induction motors are also self-started. The most important advantage is that induction motor speed can be controlled easily by controlling the input power frequency.
To understand it properly, let’s once again consider the simple coil arrangement. We learned that a rotating magnetic field is produced due to the 3 phase input power. It is quite clear that the speed of the RMF is proportional to the frequency of the input power. Because the rotor always tries to catch up with the RMF, the rotor speed is also proportional to frequency of the A.C power.
Thus by using a variable frequency drive, one can control the speed of the induction motor very easily. This property of the induction motor makes them an attractive choice for elevators, cranes even in electric cars. Due to the high speed band of induction motors, electric cars are capable to run with a single speed transmission.
Another interesting property of the induction motor is that, when the rotor is moved by a prime mover it can also acts like a generator. In this case you have to make sure that the RMF speed is always less than the rotor speed.
We believe that you have now developed a clear understanding of the ingenious operation principles behind an induction motor, as well as why it is still ruling the domestic and industrial worlds.