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What is induction motor 
OAn induction motor is an AC 
electric motor in which the electric 
current in the rotor needed to produce 
torque is obtained by 
electromagnetic induction from the 
magnetic field of the stator winding.
Working principle of induction 
motor 
O When ac supply is given to the stator 
winding of induction motor, the 
alternating current starts flowing through 
the stator or main winding. This 
alternating current produces an 
alternating flux called main flux. This 
main flux also links with the rotor 
conductors and hence cut the rotor 
conductor.
FARADAY’S LAW OF ELECTROMAGNETIC 
INDUCTION 
According to the Faraday’s law of electromagnetic induction, emf gets 
induced in the rotor. As the rotor circuit is closed one so, the current starts 
flowing in the rotor. This currents called the rotor current. This 
rotor current produces its own flux called rotor flux. Since this flux is 
produced due to induction principle so, the motor working on this 
principle got its name as induction motor. Now there are two fluxes one is 
main flux and another is called rotor flux. These two fluxes produce the 
desired torque which is required by the motor to rotate.
 Induction motors are used worldwide in 
many residential, commercial, industrial, 
and utility applications. 
 Induction Motors transform electrical 
energy into mechanical energy. 
 It can be part of a pump or fan, or 
connected to some other form of 
mechanical equipment such as a winder, 
conveyor, or mixer.
It consists of two parts: 
1. Stator - It is the stationary part of the 
motor. 
2. Rotor - It is the rotating part of the 
motor.
STATOR
Stator has three main parts: 
Outer Frame – It is the outer body of the of the 
motor. It protects the inner part of the machine. 
Stator Core – Built up of high grade silicon steel. 
Carries the alternating magnetic field 
Stator winding – Has a three phase winding.
CORE 
WINDINGS 
SLOTS
Effect of 3 Phase Current Passing Through a 
Stator Winding: 
When a 3 phase AC current passes through the 
winding It produces a rotating magnetic 
field (RMF). As shown in the figure below a 
magnetic field is produced which is rotating in 
nature. We will see how this is produced in the 
next section.
The Concept of a Rotating 
Magnetic Field 
To understand a rotating magnetic field, we 
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. 
Due to the variation in the A.C current, the 
magnetic field also varies in orientation and its 
magnitude remains the same. 
The speed of rotation of the magnetic field is 
known as synchronous speed.
The Effect of RMF on a Closed 
Conductor 
Assume we 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. 
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.
ROTOR
There are two types of rotors which are 
employed in 3 – phase induction motor. 
Squirrel Cage Rotor. 
Phase Wound/ Slip Ring Rotor.
SQUIRREL CAGE 
ROTOR
It consists of a laminated cylindrical core 
having semi closed circular slots at the outer 
periphery. 
Copper or aluminum bar conductors are 
placed in these slots and short circuited at 
each end by copper or aluminum rings called 
short circuiting rings. 
The rotor winding is permanently short 
circuited and it is not possible to add any 
external resistance.
The rotor slots are not parallel to the shaft 
but skewed to 
Reduce humming . 
 Provide smoother torque for different 
positions of rotor. 
Reduce magnetic locking of stator and 
rotor.
PHASE 
WOUND 
ROTOR
It is also called SLIP RING ROTOR. 
 Consists of a laminated core having semi 
closed slots at the outer periphery and 
carries a 3-phase insulated winding. 
 The rotor is wound for the same number of 
poles as that of stator. 
 The three finish terminals are connected 
together forming a star point and the three 
star terminals are connected to three slip 
rings fixed on the shaft.
Construction (Enclosure) 
 The enclosure consists of a frame (or yoke) and 
two end brackets (or bearing housings). The stator 
is mounted inside the frame. 
 The rotor fits inside the stator with a slight air gap 
separating it from the stator. There is NO direct 
physical connection between the rotor and the 
stator.
 The enclosure also protects the electrical and 
operating parts of the motor from harmful effects of 
the environment in which the motor operates. 
Bearings, mounted on the shaft, support the rotor 
and allow it to turn. A fan, also mounted on the 
shaft, is used on the motor shown below for 
cooling.
Stator 
Rotor 
Air gap
The Working of an Induction Motor 
A 3-phase AC current passing through a Stator winding 
produces a rotating magnetic field. 
current will be induced in the bars of the squirrel cage and it 
will start to rotate. 
We 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.
which is the most commonly 
used one in induction motors.
RMF produces a 
torque on rotor as 
in the simple 
winding case.
Poles and speed 
O Every ac induction motor has poles, just like a magnet. However, 
unlike a simple magnet, these poles are formed by bundles of 
magnet wire (windings) wound together in slots of the stator core.In 
most cases, you can look inside the motor and count the number of 
poles in the winding; they are distinct bundles of wire evenly spaced 
around the stator core. 
O The number of poles, combined with the ac line frequency (Hertz, 
Hz), are all that determine the no-load revolutions per minute (rpm) 
of the motor. So, all four-pole motors will run at the same speed 
under no-load conditions, all six-pole motors will run at the same 
speed, and so on. 
O The mathematical formula to remember in helping make this 
calculation is the number of cycles (Hz) times 60 (for seconds in a 
minute) times two (for the positive and negative pulses in the cycle) 
divided by the number of poles.
 Therefore, for a 60-Hz system, the formula would be: 
60 x 60 x 2 = 7,200 no-load rpm ÷ number of poles. 
 For a 50-Hz system, the formula would be: 
50 x 60 x 2 = 6,000 no-load rpm ÷ number of poles. 
 Using this formula, you can see that a four-pole motor 
operating on the bench under no-load conditions runs at 1,800 
rpm (7,200 ÷ 4 poles). Note that when an ac motor is loaded, 
the spinning magnetic field in the stator does not change 
speed. Instead, the rotor or moving part of the motor is 
restrained by the load from “catching up” to the field speed. 
 The difference between the field speed of 1,800 rpm in this 
example and the rotor speed of approximately 1,725 rpm is 
called the “slip.” Slip varies with the load over a narrow 
operating range for each motor design.
 Motor Speeds, Both Loaded and Unloaded 
 Our spinning four-pole motor, then, operates at 1,800 rpm in 
this example under no-load conditions and approximately 
1,725 rpm under load. Motors of this speed are commonly 
found in belted applications such as blowers, fans, air-handling 
equipment, compressors, and some conveyors .A 
two-pole motor operates at 3,600 rpm (7,200 rpm ÷ 2) 
unloaded, and approximately 3,450 under load. Two-pole 
motors often are found in pump applications, such as sump 
pumps, swimming pool pumps, and water re circulating 
equipment. 
 One thing for the service technician to keep in mind in the 
field is that the higher the rpm, the noisier a motor may sound 
to the untrained ear. It is beneficial to become aware of the 
different speed-related sounds motors make. 
 found in ceiling fans.
O Six-pole motors run at 1,200 rpm unloaded (7,200 ÷ 6) 
and between 1,050 and 1,175 rpm loaded. They are often 
used for air-handling equipment, direct-drive 
applications, window fans, furnace blowers, room air 
conditioners, heat pumps, and other equipment where 
the relatively slower motor speed makes for quieter 
operation. All can come in either totally open, totally 
enclosed, or combination models, adding to their 
versatility. 
O To satisfy consumers’ desires for quieter motors, 
manufacturers have developed eight-pole motors. These 
operate at 900 rpm (unloaded) and approximately 800 
rpm under load. They are being used in applications 
where customers expect quieter operation, such as room 
air conditioners and outdoor heat pump applications. 
O Less-common pole configurations include 12-pole 
motors (600 rpm) that are used in applications requiring 
slow speeds, such as washing machines, and 16-pole 
motors (450 rpm unloaded), often found in
electricity is induced in rotor by magnetic 
induction rather than direct electric 
connection , That's why the name induction 
motor is used. 
To aid such electromagnetic induction, 
insulated iron core lamina are packed inside 
the rotor.
Thin layers of iron lamina which are 
packed in rotor
The Speed of Rotation of a Rotor 
Both the magnetic field and rotor are rotating. 
To find the speed of the rotor let's consider 
different cases.
Consider a case where the rotor speed is 
same as the magnetic field speed. 
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.
Slip 
The difference between the flux (Ns) and the 
rotor speed (N) is called slip. 
 % Slip = (Ns – N) × 100 
Slip speed = Ns – N
Energy Transfer in the Motor 
In an induction motor, electrical energy is enters 
via the Stator and output from the rotor, 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.
A cooling fan is used to remove heat 
liberated by motor
SPEED CONTROL OF AN INDUCTION MOTOR 
The speed of an induction motor can be easily 
controlled by varying the frequency of the 3-phase 
supply. 
To maintain a constant (rated) flux density, the applied 
voltage must also be changed in the same proportion as 
the frequency (as dictated by Faraday’s law). 
This speed control method is known as Volts per Hz. 
 Above rated speed, the applied voltage is usually kept 
constant at rated value; this operation is referred to as 
constant HP. At low frequencies (i.e. speeds), the voltage 
must be boosted in order to compensate for the effects of 
the stator resistance.
Advantages and disadvantages of 
induction motors 
“Advantages” 
 They have only one moving part, the rotor, 
which makes them low-cost, quiet, long-lasting, 
and relatively trouble free. 
DC motors, by contrast, have a commutator and 
carbon brushes that wear out and need replacing 
from time to time. 
 The friction between the brushes and the 
commutator also makes DC motors relatively noisy 
(and sometimes even quite smelly).
“Disadvantages” 
Since the speed of an induction motor depends on the 
frequency of the alternating current that drives it, it turns at a 
constant speed unless you use a variable-frequency drive. 
 the speed of DC motors is much easier to control simply by 
turning the supply voltage up or down. 
Induction motors can be fairly heavy because of their coil 
windings. 
 Unlike DC motors, they can't be driven from batteries or 
any other source of DC power without using an inverter. 
That's because they need a changing magnetic field to turn 
the rotor.
Induction motor
Induction motor

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Induction motor

  • 1.
  • 2. What is induction motor OAn induction motor is an AC electric motor in which the electric current in the rotor needed to produce torque is obtained by electromagnetic induction from the magnetic field of the stator winding.
  • 3. Working principle of induction motor O When ac supply is given to the stator winding of induction motor, the alternating current starts flowing through the stator or main winding. This alternating current produces an alternating flux called main flux. This main flux also links with the rotor conductors and hence cut the rotor conductor.
  • 4. FARADAY’S LAW OF ELECTROMAGNETIC INDUCTION According to the Faraday’s law of electromagnetic induction, emf gets induced in the rotor. As the rotor circuit is closed one so, the current starts flowing in the rotor. This currents called the rotor current. This rotor current produces its own flux called rotor flux. Since this flux is produced due to induction principle so, the motor working on this principle got its name as induction motor. Now there are two fluxes one is main flux and another is called rotor flux. These two fluxes produce the desired torque which is required by the motor to rotate.
  • 5.  Induction motors are used worldwide in many residential, commercial, industrial, and utility applications.  Induction Motors transform electrical energy into mechanical energy.  It can be part of a pump or fan, or connected to some other form of mechanical equipment such as a winder, conveyor, or mixer.
  • 6.
  • 7. It consists of two parts: 1. Stator - It is the stationary part of the motor. 2. Rotor - It is the rotating part of the motor.
  • 8.
  • 10. Stator has three main parts: Outer Frame – It is the outer body of the of the motor. It protects the inner part of the machine. Stator Core – Built up of high grade silicon steel. Carries the alternating magnetic field Stator winding – Has a three phase winding.
  • 12.
  • 13. Effect of 3 Phase Current Passing Through a Stator Winding: When a 3 phase AC current passes through the winding It produces a rotating magnetic field (RMF). As shown in the figure below a magnetic field is produced which is rotating in nature. We will see how this is produced in the next section.
  • 14.
  • 15. The Concept of a Rotating Magnetic Field To understand a rotating magnetic field, we 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.
  • 16.
  • 17. The components of A.C current will vary with time. Due to the variation in the A.C current, the magnetic field also varies in orientation and its magnitude remains the same. The speed of rotation of the magnetic field is known as synchronous speed.
  • 18.
  • 19. The Effect of RMF on a Closed Conductor Assume we 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. 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.
  • 20.
  • 21. ROTOR
  • 22. There are two types of rotors which are employed in 3 – phase induction motor. Squirrel Cage Rotor. Phase Wound/ Slip Ring Rotor.
  • 24. It consists of a laminated cylindrical core having semi closed circular slots at the outer periphery. Copper or aluminum bar conductors are placed in these slots and short circuited at each end by copper or aluminum rings called short circuiting rings. The rotor winding is permanently short circuited and it is not possible to add any external resistance.
  • 25.
  • 26. The rotor slots are not parallel to the shaft but skewed to Reduce humming .  Provide smoother torque for different positions of rotor. Reduce magnetic locking of stator and rotor.
  • 27.
  • 29.
  • 30. It is also called SLIP RING ROTOR.  Consists of a laminated core having semi closed slots at the outer periphery and carries a 3-phase insulated winding.  The rotor is wound for the same number of poles as that of stator.  The three finish terminals are connected together forming a star point and the three star terminals are connected to three slip rings fixed on the shaft.
  • 31. Construction (Enclosure)  The enclosure consists of a frame (or yoke) and two end brackets (or bearing housings). The stator is mounted inside the frame.  The rotor fits inside the stator with a slight air gap separating it from the stator. There is NO direct physical connection between the rotor and the stator.
  • 32.  The enclosure also protects the electrical and operating parts of the motor from harmful effects of the environment in which the motor operates. Bearings, mounted on the shaft, support the rotor and allow it to turn. A fan, also mounted on the shaft, is used on the motor shown below for cooling.
  • 34. The Working of an Induction Motor A 3-phase AC current passing through a Stator winding produces a rotating magnetic field. current will be induced in the bars of the squirrel cage and it will start to rotate. We 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.
  • 35. which is the most commonly used one in induction motors.
  • 36. RMF produces a torque on rotor as in the simple winding case.
  • 37. Poles and speed O Every ac induction motor has poles, just like a magnet. However, unlike a simple magnet, these poles are formed by bundles of magnet wire (windings) wound together in slots of the stator core.In most cases, you can look inside the motor and count the number of poles in the winding; they are distinct bundles of wire evenly spaced around the stator core. O The number of poles, combined with the ac line frequency (Hertz, Hz), are all that determine the no-load revolutions per minute (rpm) of the motor. So, all four-pole motors will run at the same speed under no-load conditions, all six-pole motors will run at the same speed, and so on. O The mathematical formula to remember in helping make this calculation is the number of cycles (Hz) times 60 (for seconds in a minute) times two (for the positive and negative pulses in the cycle) divided by the number of poles.
  • 38.  Therefore, for a 60-Hz system, the formula would be: 60 x 60 x 2 = 7,200 no-load rpm ÷ number of poles.  For a 50-Hz system, the formula would be: 50 x 60 x 2 = 6,000 no-load rpm ÷ number of poles.  Using this formula, you can see that a four-pole motor operating on the bench under no-load conditions runs at 1,800 rpm (7,200 ÷ 4 poles). Note that when an ac motor is loaded, the spinning magnetic field in the stator does not change speed. Instead, the rotor or moving part of the motor is restrained by the load from “catching up” to the field speed.  The difference between the field speed of 1,800 rpm in this example and the rotor speed of approximately 1,725 rpm is called the “slip.” Slip varies with the load over a narrow operating range for each motor design.
  • 39.  Motor Speeds, Both Loaded and Unloaded  Our spinning four-pole motor, then, operates at 1,800 rpm in this example under no-load conditions and approximately 1,725 rpm under load. Motors of this speed are commonly found in belted applications such as blowers, fans, air-handling equipment, compressors, and some conveyors .A two-pole motor operates at 3,600 rpm (7,200 rpm ÷ 2) unloaded, and approximately 3,450 under load. Two-pole motors often are found in pump applications, such as sump pumps, swimming pool pumps, and water re circulating equipment.  One thing for the service technician to keep in mind in the field is that the higher the rpm, the noisier a motor may sound to the untrained ear. It is beneficial to become aware of the different speed-related sounds motors make.  found in ceiling fans.
  • 40. O Six-pole motors run at 1,200 rpm unloaded (7,200 ÷ 6) and between 1,050 and 1,175 rpm loaded. They are often used for air-handling equipment, direct-drive applications, window fans, furnace blowers, room air conditioners, heat pumps, and other equipment where the relatively slower motor speed makes for quieter operation. All can come in either totally open, totally enclosed, or combination models, adding to their versatility. O To satisfy consumers’ desires for quieter motors, manufacturers have developed eight-pole motors. These operate at 900 rpm (unloaded) and approximately 800 rpm under load. They are being used in applications where customers expect quieter operation, such as room air conditioners and outdoor heat pump applications. O Less-common pole configurations include 12-pole motors (600 rpm) that are used in applications requiring slow speeds, such as washing machines, and 16-pole motors (450 rpm unloaded), often found in
  • 41. electricity is induced in rotor by magnetic induction rather than direct electric connection , That's why the name induction motor is used. To aid such electromagnetic induction, insulated iron core lamina are packed inside the rotor.
  • 42. Thin layers of iron lamina which are packed in rotor
  • 43. The Speed of Rotation of a Rotor Both the magnetic field and rotor are rotating. To find the speed of the rotor let's consider different cases.
  • 44. Consider a case where the rotor speed is same as the magnetic field speed. 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.
  • 45. 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.
  • 46. Slip The difference between the flux (Ns) and the rotor speed (N) is called slip.  % Slip = (Ns – N) × 100 Slip speed = Ns – N
  • 47.
  • 48. Energy Transfer in the Motor In an induction motor, electrical energy is enters via the Stator and output from the rotor, 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.
  • 49. A cooling fan is used to remove heat liberated by motor
  • 50. SPEED CONTROL OF AN INDUCTION MOTOR The speed of an induction motor can be easily controlled by varying the frequency of the 3-phase supply. To maintain a constant (rated) flux density, the applied voltage must also be changed in the same proportion as the frequency (as dictated by Faraday’s law). This speed control method is known as Volts per Hz.  Above rated speed, the applied voltage is usually kept constant at rated value; this operation is referred to as constant HP. At low frequencies (i.e. speeds), the voltage must be boosted in order to compensate for the effects of the stator resistance.
  • 51. Advantages and disadvantages of induction motors “Advantages”  They have only one moving part, the rotor, which makes them low-cost, quiet, long-lasting, and relatively trouble free. DC motors, by contrast, have a commutator and carbon brushes that wear out and need replacing from time to time.  The friction between the brushes and the commutator also makes DC motors relatively noisy (and sometimes even quite smelly).
  • 52. “Disadvantages” Since the speed of an induction motor depends on the frequency of the alternating current that drives it, it turns at a constant speed unless you use a variable-frequency drive.  the speed of DC motors is much easier to control simply by turning the supply voltage up or down. Induction motors can be fairly heavy because of their coil windings.  Unlike DC motors, they can't be driven from batteries or any other source of DC power without using an inverter. That's because they need a changing magnetic field to turn the rotor.