Induction Machine electrical and electronics

Unit-3
INDUCTION MACHINES AND SYNCHRONOUS
MACHINES
Principle of operation of three-phase induction motors –
Construction –Types – Equivalent circuit
Construction of single-phase induction motors – Types of
single phase induction motors – Double revolving field
theory – starting methods
Principles of alternator – Construction details – Types
Equation of induced EMF – Voltage regulation.
Methods of starting of synchronous motors – Torque
equation – V curves – Synchronous motors.

INDUCTION MOTOR
OVER VIEW:
 Introduction about induction motor
 Construction of three phase induction
motor
 Principle of operation of 3- phase
induction motor

Introduction
Three-phase induction motors are the most
commonly used machines in industry
◦ Simple design,
◦ Rugged,
◦ Low-cost,
◦ Easy maintenance
◦ wide range of power ratings: fractional HP to10
MW
◦ Run essentially as constant speed from no-load
to full load

Construction of 3-Phase Induction
motor
 An induction motor has two main parts
1. Stator
2. Rotor

1. Stator
Stationary part .
Consisting of Stator Frame and Core.
Stator core is made up of laminated silicon
steel stampings having the thickness of 0.3
to 0.5mm.
In core slots are provided the space for the
stator winding.
Stator winding may be star or delta
connected.

2. ROTOR
◦ Rotating part
◦ composed of punched laminations, stacked to create a series of
rotor slots, providing space for the rotor winding
TWO TYPES OF ROTOR
1.SQUIRREL-CAGE ROTOR
2. SLIP RING or WOUND-ROTOR

1.SQUIRREL-CAGE ROTOR
Made up of cylindrical laminated core with slots to
carry rotor conductors.
Rotor conductors are heavy bars of copper or
aluminum shorted together at the both ends by two
aluminum rings, forming a squirrel-cage shaped
circuit (squirrel-cage)

2. SLIP RING or WOUND-ROTOR
 Similar to the winding on the stator. (star/delta)
 The 3-phases are brought out and connected to slip
rings mounted on the rotor shaft
 Variable external resistance can be connected in the
rotor circuit, with help of brushes and slip ring
arrangements.
 by varying the external resistance the motor speed
and torque can be controlled.

Types of 3-phase induction
motor
1. Squirrel cage induction motor.
2. Slip ring or wound rotor induction motor

1. Squirrel cage induction motor.

2. Slip ring or wound rotor induction motor
Brushes
Slip rings

Rotating Magnetic Field
 Balanced three phase windings, i.e.
mechanically displaced 120 degrees form
each other, fed by balanced three phase
source
 A rotating magnetic field with constant
magnitude is produced, rotating with a
speed
Where
f is the supply frequency and
P is the no. of poles and
120 e
sync
f
n rpm
P


Principle of operation
 This rotating magnetic field cuts the rotor windings
and produces an induced voltage in the rotor
windings
 Due to the fact that the rotor windings are short
circuited, for both squirrel cage and wound-rotor, and
induced current flows in the rotor windings
 The rotor current produces another magnetic field
 A torque is produced as a result of the interaction of
those two magnetic fields
Where ind is the induced torque and BR and BS are the
magnetic flux densities of the rotor and the stator
respectively
ind R s
kB B
  

Induction motor speed
 At what speed will the IM run?
◦ Can the IM run at the synchronous speed, why?
◦ If rotor runs at the synchronous speed, which is the
same speed of the rotating magnetic field, then the
rotor will appear stationary to the rotating magnetic
field and the rotating magnetic field will not cut the
rotor. So, no induced current will flow in the rotor
and no rotor magnetic flux will be produced so no
torque is generated and the rotor speed will fall
below the synchronous speed
◦ When the speed falls, the rotating magnetic field
will cut the rotor windings and a torque is produced

Induction motor speed
 So, the IM will always run at a speed
lower than the synchronous speed
 The difference between the motor
speed and the synchronous speed is
called the Slip
Where nslip= slip speed
nsync= speed of the magnetic field
nm = mechanical shaft speed of the motor
slip sync m
n n n
 

The Slip
sync m
sync
n n
s
n


Where s is the slip
Notice that : if the rotor runs at synchronous speed
s = 0
if the rotor is stationary
s = 1
Slip may be expressed as a percentage by multiplying the
above eq. by 100, notice that the slip is a ratio and doesn’t
have units

Effect of Slip on Rotor
Parameters
 Rotor Frequency(Fr)
 Rotor Induced EMF(E2r)
 Rotor Reactance(X2r)
 Rotor power factor(CosΦ2r)
 Rotor current(I2r)

Induction Motors and
Transformers
 Both IM and transformer works on the principle of
induced voltage
◦ Transformer: voltage applied to the primary
windings produce an induced voltage in the
secondary windings
◦ Induction motor: voltage applied to the stator
windings produce an induced voltage in the rotor
windings
◦ The difference is that, in the case of the induction
motor, the secondary windings can move
◦ Due to the rotation of the rotor (the secondary
winding of the IM), the induced voltage in it does
not have the same frequency of the stator (the
primary) voltage

Frequency
 The frequency of the voltage induced in
the rotor is given by
Where fr = the rotor frequency (Hz)
P = number of stator poles
n = slip speed (rpm)
120
r
P n
f


( )
120
120
s m
r
s
e
P n n
f
P sn
sf
 


 

Frequency
 What would be the frequency of the
rotor’s induced voltage at any speed nm?
 When the rotor is blocked (s=1) , the
frequency of the induced voltage is equal
to the supply frequency
 On the other hand, if the rotor runs at
synchronous speed (s = 0), the frequency
will be zero
r e
f s f


Torque
 While the input to the induction motor is
electrical power, its output is mechanical
power and for that we should know some
terms and quantities related to mechanical
power
 Any mechanical load applied to the motor
shaft will introduce a Torque on the motor
shaft. This torque is related to the motor
output power and the rotor speed
and
.
out
load
m
P
N m



2
/
60
m
m
n
rad s

 

Horse power
 Another unit used to measure
mechanical power is the horse power
 It is used to refer to the mechanical
output power of the motor
 Since we, as an electrical engineers,
deal with watts as a unit to measure
electrical power, there is a relation
between horse power and watts
746
hp watts


Synchronous speed
P 50 Hz 60 Hz
2 3000 3600
4 1500 1800
6 1000 1200
8 750 900
10 600 720
12 500 600

Example
A 208-V, 10hp, four pole, 60 Hz, Y-
connected induction motor has a full-
load slip of 5 percent
1. What is the synchronous speed of this
motor?
2. What is the rotor speed of this motor at
rated load?
3. What is the rotor frequency of this motor
at rated load?
4. What is the shaft torque of this motor at
rated load?

Solution
1.
2.
3.
4.
120 120(60)
1800
4
e
sync
f
n rpm
P
  
(1 )
(1 0.05) 1800 1710
m s
n s n
rpm
 
   
0.05 60 3
r e
f sf Hz
   
2
60
10 746 /
41.7 .
1710 2 (1/ 60)
out out
load
m
m
P P
n
hp watt hp
N m

 

 

 
 

Equivalent Circuit
 The induction motor is similar to the
transformer with the exception that its
secondary windings are free to rotate
As we noticed in the transformer, it is easier if we
can combine these two circuits in one circuit but

Equivalent Circuit
 When the rotor is locked (or blocked), i.e.
s =1, the largest voltage and rotor
frequency are induced in the rotor, Why?
 On the other side, if the rotor rotates at
synchronous speed, i.e. s = 0, the
induced voltage and frequency in the rotor
will be equal to zero, Why?
Where ER0 is the largest value of the rotor’s
induced voltage obtained at s = 1(loacked
0
R R
E sE


Equivalent Circuit
 The same is true for the frequency, i.e.
 It is known that
 So, as the frequency of the induced
voltage in the rotor changes, the reactance
of the rotor circuit also changes
Where Xr0 is the rotor reactance
at the supply frequency
(at blocked rotor)
r e
f s f

2
X L f L
 
 
0
2
2
r r r r r
e r
r
X L f L
sf L
sX
 

 



Equivalent Circuit
 Then, we can draw the rotor
equivalent circuit as follows
Where ER is the induced voltage in the rotor
and RR is the rotor resistance

Equivalent Circuit
 Now we can calculate the rotor current
as
 Dividing both the numerator and
denominator by s so nothing changes
we get
0
0
( )
( )
R
R
R R
R
R R
E
I
R jX
sE
R jsX




0
0
( )
R
R
R
R
E
I
R
jX
s



Equivalent Circuit
 Now we can have the rotor equivalent
circuit

Equivalent Circuit
 Now as we managed to solve the
induced voltage and different
frequency problems, we can combine
the stator and rotor circuits in one
equivalent circuit
Where
2
2 0
2
2
2
1 0
eff R
eff R
R
eff
eff R
S
eff
R
X a X
R a R
I
I
a
E a E
N
a
N






Power losses in Induction
machines
 Copper losses
◦ Copper loss in the stator (PSCL) = I1
2R1
◦ Copper loss in the rotor (PRCL) = I2
2R2
 Core loss (Pcore)
 Mechanical power loss due to friction
and windage
 How this power flow in the motor?

Power relations
3 cos 3 cos
in L L ph ph
P V I V I
 
 
2
1 1
3
SCL
P I R

( )
AG in SCL core
P P P P
  
2
2 2
3
RCL
P I R

conv AG RCL
P P P
 
( )
out conv f w stray
P P P P

   conv
ind
m
P




Equivalent Circuit
 We can rearrange the equivalent
circuit as follows
Actual rotor
resistance
Resistance
equivalent to
mechanical load

Power relations
3 cos 3 cos
in L L ph ph
P V I V I
 
 
2
1 1
3
SCL
P I R

( )
AG in SCL core
P P P P
  
2
2 2
3
RCL
P I R

conv AG RCL
P P P
 
( )
out conv f w stray
P P P P

  
conv RCL
P P
  2 2
2
3
R
I
s

2 2
2
(1 )
3
R s
I
s


RCL
P
s

(1 )
RCL
P s
s


(1 )
conv AG
P s P
 
conv
ind
m
P



(1 )
(1 )
AG
s
s P
s 




Power relations
AG
P
RCL
P
conv
P
1
s
1-s
: :
1 : : 1-
AG RCL conv
P P P
s s

Example
A 480-V, 60 Hz, 50-hp, three phase
induction motor is drawing 60A at
0.85 PF lagging. The stator copper
losses are 2 kW, and the rotor copper
losses are 700 W. The friction and
windage losses are 600 W, the core
losses are 1800 W, and the stray
losses are negligible. Find the
following quantities:
1. The air-gap power PAG.
2. The power converted P .

Solution
1.
2.
3.
3 cos
3 480 60 0.85 42.4 kW
in L L
P V I 

    
42.4 2 1.8 38.6 kW
AG in SCL core
P P P P
  
   
700
38.6 37.9 kW
1000
conv AG RCL
P P P
 
  
&
600
37.9 37.3 kW
1000
out conv F W
P P P
 
  

Solution
4.
37.3
50 hp
0.746
out
P  
100%
37.3
100 88%
42.4
out
in
P
P
  
  

Example
A 460-V, 25-hp, 60 Hz, four-pole, Y-connected induction
motor has the following impedances in ohms per phase
referred to the stator circuit:
R1= 0.641 R2= 0.332
X1= 1.106  X2= 0.464  XM= 26.3 
The total rotational losses are 1100 W and are assumed to
be constant. The core loss is lumped in with the
rotational losses. For a rotor slip of 2.2 percent at the
rated voltage and rated frequency, find the motor’s
1. Speed
2. Stator current
3. Power factor
4. Pconv and Pout
5. ind and load
6. Efficiency

Solution
1.
2.
120 120 60
1800 rpm
4
e
sync
f
n
P

  
(1 ) (1 0.022) 1800 1760 rpm
m sync
n s n
     
2
2 2
0.332
0.464
0.022
15.09 0.464 15.1 1.76
R
Z jX j
s
j
   
     
2
1 1
1/ 1/ 0.038 0.0662 1.76
1
12.94 31.1
0.0773 31.1
f
M
Z
jX Z j
 
    
    
 

Solution
3.
4.
0.641 1.106 12.94 31.1
11.72 7.79 14.07 33.6
tot stat f
Z Z Z
j
j
 
     
     
1
460 0
3 18.88 33.6 A
14.07 33.6
tot
V
I
Z

 
    
 
cos33.6 0.833 lagging
PF   
3 cos 3 460 18.88 0.833 12530 W
in L L
P V I 
     
2 2
1 1
3 3(18.88) 0.641 685 W
SCL
P I R
   
12530 685 11845 W
AG in SCL
P P P
    

Solution
5.
6.
(1 ) (1 0.022)(11845) 11585 W
conv AG
P s P
    
& 11585 1100 10485 W
10485
= 14.1hp
746
out conv F W
P P P
    

11845
62.8 N.m
1800
2
60
AG
ind
sync
P

 
  

10485
56.9 N.m
1760
2
60
out
load
m
P

 
  

10485
100% 100 83.7%
12530
out
in
P
P
     

Torque, power and Thevenin’s
Theorem
 Thevenin’s theorem can be used to
transform the network to the left of
points ‘a’ and ‘b’ into an equivalent
voltage source VTH in series with
equivalent impedance RTH+jXTH

Theorem
1 1
( )
M
TH
M
jX
V V
R j X X


 
1 1
( )//
TH TH M
R jX R jX jX
  
2 2
1 1
| | | |
( )
M
TH
M
X
V V
R X X


 

Theorem
 Since XM>>X1 and XM>>R1
 Because XM>>X1 and XM+X1>>R1
1
M
TH
M
X
V V
X X



2
1
1
1
M
TH
M
TH
X
R R
X X
X X
 
  

 


Theorem
Then the power converted to mechanical
(Pconv)
2 2
2
2
2
( )
TH TH
T
TH TH
V V
I
Z R
R X X
s
 
 
  
 
 
2 2
2
(1 )
3
conv
R s
P I
s


And the internal mechanical torque (Tconv)
conv
ind
m
P



(1 )
conv
s
P
s 


2 2
2
3
AG
s s
R
I
P
s
 
 

Theorem
2
2
2
2
2
2
3
( )
TH
ind
s
TH TH
V R
s
R
R X X
s


 
 
   
  
 
 
 
 
  
 
 
 
 
2 2
2
2
2
2
3
1
( )
TH
ind
s
TH TH
R
V
s
R
R X X
s


 
 
 

 
  
 
 

Torque-speed characteristics
Typical torque-speed characteristics of induction motor

Comments
1. The induced torque is zero at
synchronous speed. Discussed
earlier.
2. The curve is nearly linear between
no-load and full load. In this range,
the rotor resistance is much greater
than the reactance, so the rotor
current, torque increase linearly with
the slip.
3. There is a maximum possible torque

Comments
4. The starting torque of the motor is
slightly higher than its full-load
torque, so the motor will start carrying
any load it can supply at full load.
5. The torque of the motor for a given
slip varies as the square of the
applied voltage.
6. If the rotor is driven faster than
synchronous speed it will run as a
generator, converting mechanical

Maximum torque
 Maximum torque occurs when the
power transferred to R2/s is maximum.
 This condition occurs when R2/s
equals the magnitude of the
impedance RTH + j (XTH + X2)
max
2 2
2
2
( )
TH TH
T
R
R X X
s
  
max
2
2 2
2
( )
T
TH TH
R
s
R X X

 

Maximum torque
 The corresponding maximum torque of an
induction motor equals
The slip at maximum torque is directly
proportional to the rotor resistance R2
The maximum torque is independent of R2
2
max 2 2
2
3
1
2 ( )
TH
s TH TH TH
V
R R X X


 
 

 
  
 

Maximum torque
 Rotor resistance can be increased by
inserting external resistance in the rotor of
a wound-rotor induction motor.
The
value of the maximum torque remains
unaffected
but
the speed at which it occurs can be
controlled.

Maximum torque
Effect of rotor resistance on torque-speed characteristic

Example
A two-pole, 50-Hz induction motor supplies
15kW to a load at a speed of 2950 rpm.
1. What is the motor’s slip?
2. What is the induced torque in the motor
in N.m under these conditions?
3. What will be the operating speed of the
motor if its torque is doubled?
4. How much power will be supplied by the
motor when the torque is doubled?

Solution
1.
2.
120 120 50
3000 rpm
2
3000 2950
0.0167 or 1.67%
3000
e
sync
sync m
sync
f
n
P
n n
s
n

  
 
  
3
no given
assume and
15 10
48.6 N.m
2
2950
60
f W
conv load ind load
conv
ind
m
P
P P
P
 




  

  


Solution
3. In the low-slip region, the torque-speed
curve is linear and the induced torque is
direct proportional to slip. So, if the
torque is doubled the new slip will be
3.33% and the motor speed will be
4.
(1 ) (1 0.0333) 3000 2900 rpm
m sync
n s n
     
2
(2 48.6) (2900 ) 29.5 kW
60
conv ind m
P  


    

Example
A 460-V, 25-hp, 60-Hz, four-pole, Y-
connected wound-rotor induction motor
has the following impedances in ohms
per phase referred to the stator circuit
R1= 0.641 R2= 0.332
X1= 1.106  X2= 0.464  XM= 26.3 
1. What is the maximum torque of this
motor? At what speed and slip does it
occur?
2. What is the starting torque of this
motor?
3. If the rotor resistance is doubled, what is

Solution
2 2
1 1
2 2
( )
460
26.3
3 255.2 V
(0.641) (1.106 26.3)
M
TH
M
X
V V
R X X


 

 
 
2
1
1
2
26.3
(0.641) 0.590
1.106 26.3
M
TH
M
X
R R
X X
 
  

 
 
  
 

 
1 1.106
TH
X X
  

Solution
1.
The corresponding speed is
max
2
2 2
2
2 2
( )
0.332
0.198
(0.590) (1.106 0.464)
T
TH TH
R
s
R X X

 
 
 
(1 ) (1 0.198) 1800 1444 rpm
m sync
n s n
     

Solution
The torque at this speed is
2
max 2 2
2
2
2 2
3
1
2 ( )
3 (255.2)
2
2 (1800 )[0.590 (0.590) (1.106 0.464) ]
60
229 N.m
TH
s TH TH TH
V
R R X X



 
 

 
  
 


    


Solution
2. The starting torque can be found from
the torque eqn. by substituting s = 1
 
2 2
2
1
2
2
2
1
2
2
2 2
2 2
2
2 2
3
1
( )
3
[ ( ) ]
3 (255.2) (0.332)
2
1800 [(0.590 0.332) (1.106 0.464) ]
60
104 N.m
TH
start ind s
s
TH TH
s
TH
s TH TH
R
V
s
R
R X X
s
V R
R R X X
 





 
 
 
 
 
  
 
 

  
 

    


Solution
3. If the rotor resistance is doubled, then
the slip at maximum torque doubles too
The corresponding speed is
The maximum torque is still
max = 229 N.m
max
2
2 2
2
0.396
( )
T
TH TH
R
s
R X X
 
 
(1 ) (1 0.396) 1800 1087 rpm
m sync
n s n
     

Solution
The starting torque is now
2
2 2
3 (255.2) (0.664)
2
1800 [(0.590 0.664) (1.106 0.464) ]
60
170 N.m
start


 

    


Determination of motor
parameters
 Due to the similarity between the
induction motor equivalent circuit and
the transformer equivalent circuit,
same tests are used to determine the
values of the motor parameters.
◦ DC test: determine the stator resistance
R1
◦ No-load test: determine the rotational
losses and magnetization current (similar
to no-load test in Transformers).
◦ Locked-rotor test: determine the rotor and

DC test
◦ The purpose of the DC test is to determine
R1. A variable DC voltage source is
connected between two stator terminals.
◦ The DC source is adjusted to provide
approximately rated stator current, and the
resistance between the two stator leads is
determined from the voltmeter and ammeter
readings.

DC test
◦ then
◦ If the stator is Y-connected, the per phase
stator resistance is
◦ If the stator is delta-connected, the per
phase stator resistance is
DC
DC
DC
V
R
I

1
2
DC
R
R 
1
3
2
DC
R R


No-load test
1. The motor is allowed to spin freely
2. The only load on the motor is the friction
and windage losses, so all Pconv is
consumed by mechanical losses
3. The slip is very small

No-load test
4. At this small slip
The equivalent circuit reduces to…
2 2
2 2
(1 ) R (1 )
&
R s s
R X
s s
 

No-load test
5. Combining Rc & RF+W we get……

No-load test
6. At the no-load conditions, the input
power measured by meters must equal
the losses in the motor.
7. The PRCL is negligible because I2 is
extremely small because R2(1-s)/s is
very large.
8. The input power equals
Where
&
2
1 1
3
in SCL core F W
rot
P P P P
I R P
  
 
&
rot core F W
P P P
 

No-load test
9. The equivalent input impedance is thus
approximately
If X1 can be found, in some other fashion,
the magnetizing impedance XM will be
known
1
1,
eq M
nl
V
Z X X
I

  

Blocked-rotor test
 In this test, the rotor is locked or blocked
so that it cannot move, a voltage is
applied to the motor, and the resulting
voltage, current and power are
measured.

Blocked-rotor test
 The AC voltage applied to the stator is
adjusted so that the current flow is
approximately full-load value.
 The locked-rotor power factor can be
found as
 The magnitude of the total impedance
cos
3
in
l l
P
PF
V I

 
LR
V
Z
I



Blocked-rotor test
Where X’1 and X’2 are the stator and rotor
reactances at the test frequency
respectively
'
cos sin
LR LR LR
LR LR
Z R jX
Z j Z
 
 
 
1 2
' ' '
1 2
LR
LR
R R R
X X X
 
 
2 1
LR
R R R
 
'
1 2
rated
LR LR
test
f
X X X X
f
  

Blocked-rotor test
X1 and X2 as function of XLR
Rotor Design X1 X2
Wound rotor 0.5 XLR 0.5 XLR
Design A 0.5 XLR 0.5 XLR
Design B 0.4 XLR 0.6 XLR
Design C 0.3 XLR 0.7 XLR
Design D 0.5 XLR 0.5 XLR

Example
The following test data were taken on a 7.5-hp, four-pole, 208-V,
60-Hz, design A, Y-connected IM having a rated current of 28 A.
DC Test:
VDC = 13.6 V IDC = 28.0 A
No-load Test:
Vl = 208 V f = 60 Hz
I = 8.17 A Pin = 420 W
Locked-rotor Test:
Vl = 25 V f = 15 Hz
I = 27.9 A Pin = 920 W
(a) Sketch the per-phase equivalent circuit of this motor.
(b) Find the slip at pull-out torque, and find the value of the pull-out
torque.

Induction Machine electrical and electronics

More Related Content

What's hot (20)

Similar to Induction Machine electrical and electronics (20)

More from prakashpacet (8)

Recently uploaded (20)

Induction Machine electrical and electronics