Cogging and Crawling Effect in Induction Motor

 

What is Cogging in Induction Motor?

Cogging of induction motors is defined as the tendency of an induction motor to become magnetically locked, which will occur when the number of slots on the stator and rotor are equal or integral multiple of each other.

If the number of slots on the stator (S1) is equal or integral multiple of the number of slots on the rotor (S2) then the reluctance offered by the air gap is quite pronounced, resulting in the strong alignment forces between stator and rotor teeth. These alignment forces may create an alignment torque. This torque dominates the accelerating torque or starting torque of the motor resulting in the failure of starting of the induction motor. This phenomenon is called the magnetic locking or cogging of an induction motor. 

Cogging particularly occurs in squirrel cage rotor induction motor. Because in these motors, external resistance cannot be added to get high starting torque therefore, we have to choose a reduced voltage starting method to start the induction motor. Due to reduced voltage starting the starting torque of squirrel cage induction motors is low and the alignment forces between stator and the rotor teeth dominate the starting torque of the induction motor.

In slip ring rotor induction motors, there is no need of reduced voltage starting method to get high starting torque, instead of this we can get high starting torque by adding external resistances to the rotor circuit by means of slip rings. Therefore, cogging will not occur in slip ring induction motors.

 

How to reduce Cogging in Induction Motor?

To reduce cogging of induction motors, the rotor slots are essentially skewed (also discussed in squirrel cage rotor) and the number of rotor slots will be made different from the number of stator slots, there is no common factor between them such as equal or integral multiple. 

Skewing means, shifting the rotor slots at some angle from the rotor shaft axis as shown in the given figure. Skewing of rotor slots also improves the flux distribution, reduces the harmonic content and produces better torque which makes the motor run smoothly with less noise called magnetic humming. (That's why slip ring induction motor’s rotors are also skewed).

Cogging in Induction Motor



What is Crawling in Induction Motor?


Crawling of an induction motor refers to the running of the motor stably at low speed i.e. Ns/7. This happens due to the influence of 7th harmonic frequency MMF distribution. Crawling is undesirable for an induction motor because at such low speed the slip of the induction motor is significantly high causing the motor to draw high current and produce large noise.

As we know, the flux distribution in the air gap of the induction motor is sinusoidal (ɸ = ɸm sin(ωt)). However, due to the certain combination of un-skewed stator slots and rotor slots, this flux distribution in the air gap is non sinusoidal or distorted. This distorted flux distribution contains components of fundamental plus higher order harmonic frequencies. These higher order harmonics fluxes in the air gap are undesirable and may impact the motor performance. 

Generally, even-order harmonics are not so dangerous because their average value is zero. But odd order harmonics such as 3rd, 5th, 7th, 9th,11th etc. can significantly affect the performance of induction motors (specifically 5th and 7th harmonics).

As we know, in three phase induction motor the fundamental components of flux distribution is 

ɸ= ɸm sin(ωt),           ɸb  = ɸm sin (ωt - 120),          ɸc  = ɸm sin (ωt - 240)

 

5th harmonic component of these flux waves are

ɸa  = ɸm sin5ωt,           ɸb  = ɸm sin 5(ωt - 120),          ɸc  = ɸm sin 5(ωt - 240)

ɸa  = ɸm sin5ωt,           ɸb  = ɸm sin (5ωt - 600),          ɸc  = ɸm sin (5ωt - 1200)

ɸa  = ɸm sin5ωt,           ɸb  = ɸm sin (5ωt - 240),          ɸc  = ɸm sin (5ωt - 120)

 

If we carefully observe the above flux distribution equations of the fifth harmonic frequency component, we find that these flux distributions have three phase nature, but their phase sequence is opposite to the original phase sequence. As a result, this flux rotates backward with the synchronous speed of Ns/5. Hence, this harmonic has no effect on the induction motor during the motoring zone, but it has a significant effect on the breaking zone of the induction motor. 

 

As the synchronous speed of this harmonics flux distribution is Ns5 = Ns/5. Therefore, the slip is s5 = 6/5.

 

7th harmonic component of these flux waves are

ɸa  =  ɸm sin7ωt,           ɸb  =  ɸm sin 7(ωt - 120),           ɸc  =  ɸm sin 7(ωt - 240)

ɸa  =  ɸm sin7ωt,           ɸb  =  ɸm sin (7ωt - 840),           ɸc  =  ɸm sin (7ωt - 1680)

ɸa  =  ɸm sin7ωt,            ɸb  = ɸm sin (7ωt -120),            ɸc  =  ɸm sin (7ωt - 240)

 

After carefully observing the above flux distribution equations of 7th harmonic, we find that this flux distribution has three phase nature with the phase sequence being the same as the original phase sequence. As a result, this flux rotates in the forward direction with the synchronous speed of Ns/7. Hence, this harmonic impacts the performance of an induction motor during the motoring zone. 

For this harmonic flux, the synchronous speed is Ns7 = Ns/7 and the slip is s5 = 6/7.

The above discussed harmonics i.e. 5th and 7th, generate their own asynchronous torque of the same general torque-slip curve shape as that of the fundamental. 

The given figure shows the torque slip characteristic of a three-phase induction motor with the effect of 5th and 7th harmonics frequency.

crawling of induction motor


In the given figure, we see that due to the presence of 7th harmonic content a dip in the resultant of the torque slip curve of the three-phase induction motor is introduced in the motor motoring zone. 

Therefore, if the induction motor starts with reduced voltage starting (accelerated slowly to required load torque, indicated by red dotted curve) then this effect will dominate at a point A and make the motor run at stably at speed that is Ns/7. 

At such a low speed, the slip of the induction motor is very high causing the motor to draw high current and make a large noise, which is not desired.

Similar to cogging, crawling also occurs in squirrel cage induction motors because in this type of induction motor we have to apply reduced voltage starting (starting torque is low).

Whereas in slip ring induction motor starting torque is high, so there is no crawling effect.

 

How to reduce Crawling in Induction Motor?

To minimize crawling of an induction motor, semi closed or closed slots are preferred over open slots, and the rotor slots are essentially skewed. This practice ensured a uniformly distributed air gap across the entire rotor length. This will ensure the uniform flux distribution. Additionally, short pitched windings are preferred to further enhance uniform flux distribution.

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