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Synchronous Generators
Synchronous Generators
Dr. Francis M. Fernandez
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 1
Jan 2020
Synchronous Generators
 Synchronous generator is the common type
used in generating stations
 It runs at constant speed and generates
constant frequency output
 The filed poles are on the rotor side and the
armature is on stator side
 The armature winding is placed in the slots
on stator core
 Field poles are excited with a dc supply
 DC supply to the filed poles are given
through a pair of slip rings
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 2
EXCITER
GENERATOR
TURBINE
Types of Construction
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 3
Salient Pole type Cylindrical Rotor type
N
S
S
N
Field
winding
Field pole
Armature
conductors
N
S
Stator
Cylindrical
rotor
Why Armature on Stator?
 Power in the field system is much less
compared to the generated power,
which is easily handled by the slip
rings.
 When the armature is on the stator
side, generated power is directly taken
out without the help of slip rings.
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 4
N
S
Excitation
Voltage
Slip
Rings
Stator
Windings
Relation between Speed and Frequency
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 5
N
S
A
A’
N
S
S
N
A
A’
1 revolution per second (RPS)
makes 1 Hertz
1 revolution per second (RPS)
makes 2 Hertz
2 Pole 4 Pole General case
2 f
RPS
P

where is the freuency
and is the number of poles
f
P
120
,
f
RPM N
P

Synchronous Speed
 Synchronous speed is the speed at which the generator should run to
produce a constant frequency
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 6
- freuency
- number of poles
- speed in RPM
f
P
N
Number of cycles per revolution
2
Revolution per second
60
Cycles per second
2 60 2 60
120
,
P
N
P N P N
f
f
RPM N
P


 
  
 

N
S
S
N
A
A’
Three Phase Generator
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 7
N
S
R'
Y
B
R
Y' B'
120o
 There will be three sets of similar
windings
 Windings are placed 120 degrees apart
 Practically each phase winding will be
distributed across several slots
Practical Winding
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 8
Single Layer Winding
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 9
Winding example (Full pitch)
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 10
No of poles: 2, No of slots: 12, Double layer → Slots/pole/phase = 12/(2x3) = 2
N
S
Winding example (Full pitch)
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 11
3 phase
2 pole
12 slot
Double layer winding
Winding example (Short Chorded)
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 12
No of poles: 2, No of slots: 12, Double layer → Slots/pole/phase = 12/(2x3) = 2
N
S
Winding example (Short Chorded)
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 13
3 phase
2 pole
12 slot
Double layer winding
Features of Short Chording
 Saves copper in end connections
 Improve wave shape (reduce harmonics)
 Reduce losses – both copper loss and core loss
 Reduced voltage compared to full pitch
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 14
N
S
Slot Angle
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 15
180
Slot angle =
Slots/pole N
S
180
Slot angle = 30
6
 
In this case (2 pole, 12 slot):
For a 4 pole 36 slot machine:
180
Slot angle = 20
9
 
Pitch Factor
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 16
If the coil is full pitched,
Total induced voltage in a coil = 2E
Let the voltage induced in a conductor is E
If the coil is short pitched by an angle
Total induced voltage = 2 E cos
2


Pitch Factor
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 17
If the coil is full pitched,
Total induced voltage in a coil = 2E
Let the voltage induced in a conductor is E
If the coil is short pitched by an angle
Total induced voltage = 2 cos
2
E


c
Resultant emf of chorded coil
Pitch factor,
Resultant emf of full piched coil
2 cos
2
= cos
2 2
K
E
E




Also known as coil span factor
Distribution factor
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 18
d
emf with distributed winding
Distribution facor,
emf with concentrated winding
K 
180
Slot angle, =
Slots/pole

= Slots/pole/phase
m
= phase spread angle
m
N
S
Distribution factor
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 19
d
emf with distributed winding
Distribution facor,
emf with concentrated winding
K 
AB = 2 sin
2
r


Arithematic sum = 2 sin
2
m r

Vector sum = 2 sin
2
m
r

d
2 sin sin
2 2
=
2 sin sin
2 2
m m
r
K
m r m
 
 

Example
For a 3 phase 36 slot 4 pole winding find the distribution factor
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 20
180 180
Slot angle, = 20
Slots per pole 9
   
36
Slots/pole/phase, 3
4 3
m  

d
3 20
sin sin
2 2
Distribution factor, = 0.956
20
sin 3 sin
2 2
m
K
m



 
EMF Equation
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 21
Number of coil sides in series per phase
Number of poles
Frequency
Speed in RPM
Flux per pole
Z
P
f
N




 
In one revolution each conductor is cut by webers
P

d P
  
60
dt
N
 Average emf induced volts
60 60
d P NP
dt
N
  
  
Substituting for N
120
Average emf induced 2 volts
60
P f
f
P

   
N
S
S
N
A
A’
EMF Equation
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 22
For the total winding, average emf 2
4
f Z
f T
 
 
RMS value 4.44 f T
 
Considering pitch factor and distribution factor,
c d
RMS value of per phase voltage, 4.44 volts
E K K f T
 
d
sin
2
=
sin
2
m
K
m


c cos
2
K


Example
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 23
A 4 pole 3 phase star connected alternator having 60 slots with 4 conductor per slot runs at
1500 rpm. Coils are short pitched by 3 slots. If the phase spread is 60 degrees, find the line
voltage induced fir for a flux per pole of 0.75 Wb distributed sinusoidally in space. All turns per
phase are in series.
60
Slots/pole/phase, 5
4 3
m  

180 180
Slot angle, = 12
Slots/pole 15
   
 
Coil pitch 15 3 12 144
      
Short chording angle, 180 144 36
    
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 24
60 4
Number of turns, 40
2 3
T

 

d
5 12
sin sin
2 2
= 0.957
12
sin 5 sin
2 2
m
K
m



 

c
36
cos cos 0.951
2 2
K

  
c d
Per phase voltage 4.44
4.44 0.951 0.957 0.75 50 40 6061.3 volts
K K f T
 
      
ph
Line voltage 3
3 6061.3 10498.5 volts
V
 
  
Harmonics
 Defined as sinusoidal voltages and currents at
frequencies other than the fundamental frequency.
 Harmonic frequencies are integer multiples of the
fundamental frequency
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 25






0
0 )]
sin(
)
cos(
[
)
(
n
n
n nx
b
nx
a
a
x
f
Kc and Kd for Harmonic Frequencies
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 26
dn
sin
2
=
sin
2
mn
K
n
m


cn cos
2
n
K


where is the harmonic order
n
if = 5 and = 36
n   c5
5 36
cos 0
2
K

 
Short chording can help to eliminate harmonics
Line voltage with harmonics in generated emf
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 27
VRY = VR - VY
Phase voltage
Line voltage
Third Harmonic
voltages
Line voltage with harmonics in generated emf
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 28
Phase voltage
Line voltage
Third Harmonic
voltages
Third harmonics cancel in line voltage
VRY = VR - VY
Slot Harmonics
4 February 2020 DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 29
 Distortion of flux occur due to variation of
reluctance between the slot area and tooth area
 Distortion of flux produce distortion in voltage
waveform which is known as slot harmonics
 Slot harmonics is reduced either by skewing of
field poles or by incorporating fractional slot
winding
Methods for Elimination of Harmonics
 120 Degrees phase spread
 Eliminates 3rd order harmonics
 Short Chording
 Eliminates 5th and 7th order harmonics
 Fractional slot winding
 Eliminates slot harmonics
 Skewing of field poles
 Eliminates slot harmonics
 Star connection
 Eliminates triplen (order 3, 9, 15 etc) harmonics
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 30
120 Degree Phase Spread Winding
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 31
60°
Fractional Slot Winding
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 32
Example
Calculate the rms value of induced voltage per phase of a 3 phase, 10 pole, 50 Hz, alternator
with 2 slots per pole per phase and 4 conductor per slot in 2 layers. The coil span is 150 degrees.
Flux per pole has a fundamental component of 0.12 Wb and a 20 % third harmonic component.
Also find the line voltage.
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 33
Slots/pole/phase, 2
m 
180 180
Slot angle, = 30
Slots/pole 6
   
 
Short chording angle, 180 150 30
    
Slots/pole 2 3 6
  
10 2 4
Number of turns, 40
2
T
 
 
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 34
d
2 30
sin sin
2 2
= 0.966
30
sin 2 sin
2 2
m
K
m



 

c
30
cos cos 0.966
2 2
K

  
c d
Per phase fundamental voltage 4.44
4.44 0.966 0.966 0.12 50 40 995 volts
K K f T
 
      
d3
2 3 30
sin sin
2 2
= 0.707
3 30
sin 2 sin
2 2
mn
K
n
m


 
 


c3
3 3 30
cos cos 0.707
2 2
K
 
  
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 35
3
0.2 0.12
0.008 Wb
3

   3 150 Hz
f 
c3 d3 3 3
Per phase third harmonic voltage 4.44
4.44 0.707 0.707 0.008 150 40 106 volts
K K f T
 
      
2 2
1 3
2 2
Per phase voltage
995 106 1000 volts
E E
 
  
Line voltage 3 995 1723.4 volts
  
DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 36
Thank You

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Alternator Basics.pdf

  • 1. Synchronous Generators Synchronous Generators Dr. Francis M. Fernandez DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 1 Jan 2020
  • 2. Synchronous Generators  Synchronous generator is the common type used in generating stations  It runs at constant speed and generates constant frequency output  The filed poles are on the rotor side and the armature is on stator side  The armature winding is placed in the slots on stator core  Field poles are excited with a dc supply  DC supply to the filed poles are given through a pair of slip rings DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 2 EXCITER GENERATOR TURBINE
  • 3. Types of Construction DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 3 Salient Pole type Cylindrical Rotor type N S S N Field winding Field pole Armature conductors N S Stator Cylindrical rotor
  • 4. Why Armature on Stator?  Power in the field system is much less compared to the generated power, which is easily handled by the slip rings.  When the armature is on the stator side, generated power is directly taken out without the help of slip rings. DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 4 N S Excitation Voltage Slip Rings Stator Windings
  • 5. Relation between Speed and Frequency DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 5 N S A A’ N S S N A A’ 1 revolution per second (RPS) makes 1 Hertz 1 revolution per second (RPS) makes 2 Hertz 2 Pole 4 Pole General case 2 f RPS P  where is the freuency and is the number of poles f P 120 , f RPM N P 
  • 6. Synchronous Speed  Synchronous speed is the speed at which the generator should run to produce a constant frequency DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 6 - freuency - number of poles - speed in RPM f P N Number of cycles per revolution 2 Revolution per second 60 Cycles per second 2 60 2 60 120 , P N P N P N f f RPM N P           N S S N A A’
  • 7. Three Phase Generator DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 7 N S R' Y B R Y' B' 120o  There will be three sets of similar windings  Windings are placed 120 degrees apart  Practically each phase winding will be distributed across several slots
  • 8. Practical Winding DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 8
  • 9. Single Layer Winding DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 9
  • 10. Winding example (Full pitch) DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 10 No of poles: 2, No of slots: 12, Double layer → Slots/pole/phase = 12/(2x3) = 2 N S
  • 11. Winding example (Full pitch) DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 11 3 phase 2 pole 12 slot Double layer winding
  • 12. Winding example (Short Chorded) DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 12 No of poles: 2, No of slots: 12, Double layer → Slots/pole/phase = 12/(2x3) = 2 N S
  • 13. Winding example (Short Chorded) DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 13 3 phase 2 pole 12 slot Double layer winding
  • 14. Features of Short Chording  Saves copper in end connections  Improve wave shape (reduce harmonics)  Reduce losses – both copper loss and core loss  Reduced voltage compared to full pitch DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 14 N S
  • 15. Slot Angle DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 15 180 Slot angle = Slots/pole N S 180 Slot angle = 30 6   In this case (2 pole, 12 slot): For a 4 pole 36 slot machine: 180 Slot angle = 20 9  
  • 16. Pitch Factor DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 16 If the coil is full pitched, Total induced voltage in a coil = 2E Let the voltage induced in a conductor is E If the coil is short pitched by an angle Total induced voltage = 2 E cos 2  
  • 17. Pitch Factor DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 17 If the coil is full pitched, Total induced voltage in a coil = 2E Let the voltage induced in a conductor is E If the coil is short pitched by an angle Total induced voltage = 2 cos 2 E   c Resultant emf of chorded coil Pitch factor, Resultant emf of full piched coil 2 cos 2 = cos 2 2 K E E     Also known as coil span factor
  • 18. Distribution factor DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 18 d emf with distributed winding Distribution facor, emf with concentrated winding K  180 Slot angle, = Slots/pole  = Slots/pole/phase m = phase spread angle m N S
  • 19. Distribution factor DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 19 d emf with distributed winding Distribution facor, emf with concentrated winding K  AB = 2 sin 2 r   Arithematic sum = 2 sin 2 m r  Vector sum = 2 sin 2 m r  d 2 sin sin 2 2 = 2 sin sin 2 2 m m r K m r m     
  • 20. Example For a 3 phase 36 slot 4 pole winding find the distribution factor DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 20 180 180 Slot angle, = 20 Slots per pole 9     36 Slots/pole/phase, 3 4 3 m    d 3 20 sin sin 2 2 Distribution factor, = 0.956 20 sin 3 sin 2 2 m K m     
  • 21. EMF Equation DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 21 Number of coil sides in series per phase Number of poles Frequency Speed in RPM Flux per pole Z P f N       In one revolution each conductor is cut by webers P  d P    60 dt N  Average emf induced volts 60 60 d P NP dt N       Substituting for N 120 Average emf induced 2 volts 60 P f f P      N S S N A A’
  • 22. EMF Equation DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 22 For the total winding, average emf 2 4 f Z f T     RMS value 4.44 f T   Considering pitch factor and distribution factor, c d RMS value of per phase voltage, 4.44 volts E K K f T   d sin 2 = sin 2 m K m   c cos 2 K  
  • 23. Example DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 23 A 4 pole 3 phase star connected alternator having 60 slots with 4 conductor per slot runs at 1500 rpm. Coils are short pitched by 3 slots. If the phase spread is 60 degrees, find the line voltage induced fir for a flux per pole of 0.75 Wb distributed sinusoidally in space. All turns per phase are in series. 60 Slots/pole/phase, 5 4 3 m    180 180 Slot angle, = 12 Slots/pole 15       Coil pitch 15 3 12 144        Short chording angle, 180 144 36     
  • 24. DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 24 60 4 Number of turns, 40 2 3 T     d 5 12 sin sin 2 2 = 0.957 12 sin 5 sin 2 2 m K m       c 36 cos cos 0.951 2 2 K     c d Per phase voltage 4.44 4.44 0.951 0.957 0.75 50 40 6061.3 volts K K f T          ph Line voltage 3 3 6061.3 10498.5 volts V     
  • 25. Harmonics  Defined as sinusoidal voltages and currents at frequencies other than the fundamental frequency.  Harmonic frequencies are integer multiples of the fundamental frequency DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 25       0 0 )] sin( ) cos( [ ) ( n n n nx b nx a a x f
  • 26. Kc and Kd for Harmonic Frequencies DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 26 dn sin 2 = sin 2 mn K n m   cn cos 2 n K   where is the harmonic order n if = 5 and = 36 n   c5 5 36 cos 0 2 K    Short chording can help to eliminate harmonics
  • 27. Line voltage with harmonics in generated emf DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 27 VRY = VR - VY Phase voltage Line voltage Third Harmonic voltages
  • 28. Line voltage with harmonics in generated emf DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 28 Phase voltage Line voltage Third Harmonic voltages Third harmonics cancel in line voltage VRY = VR - VY
  • 29. Slot Harmonics 4 February 2020 DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 29  Distortion of flux occur due to variation of reluctance between the slot area and tooth area  Distortion of flux produce distortion in voltage waveform which is known as slot harmonics  Slot harmonics is reduced either by skewing of field poles or by incorporating fractional slot winding
  • 30. Methods for Elimination of Harmonics  120 Degrees phase spread  Eliminates 3rd order harmonics  Short Chording  Eliminates 5th and 7th order harmonics  Fractional slot winding  Eliminates slot harmonics  Skewing of field poles  Eliminates slot harmonics  Star connection  Eliminates triplen (order 3, 9, 15 etc) harmonics DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 30
  • 31. 120 Degree Phase Spread Winding DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 31 60°
  • 32. Fractional Slot Winding DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 32
  • 33. Example Calculate the rms value of induced voltage per phase of a 3 phase, 10 pole, 50 Hz, alternator with 2 slots per pole per phase and 4 conductor per slot in 2 layers. The coil span is 150 degrees. Flux per pole has a fundamental component of 0.12 Wb and a 20 % third harmonic component. Also find the line voltage. DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 33 Slots/pole/phase, 2 m  180 180 Slot angle, = 30 Slots/pole 6       Short chording angle, 180 150 30      Slots/pole 2 3 6    10 2 4 Number of turns, 40 2 T    
  • 34. DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 34 d 2 30 sin sin 2 2 = 0.966 30 sin 2 sin 2 2 m K m       c 30 cos cos 0.966 2 2 K     c d Per phase fundamental voltage 4.44 4.44 0.966 0.966 0.12 50 40 995 volts K K f T          d3 2 3 30 sin sin 2 2 = 0.707 3 30 sin 2 sin 2 2 mn K n m         c3 3 3 30 cos cos 0.707 2 2 K     
  • 35. DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 35 3 0.2 0.12 0.008 Wb 3     3 150 Hz f  c3 d3 3 3 Per phase third harmonic voltage 4.44 4.44 0.707 0.707 0.008 150 40 106 volts K K f T          2 2 1 3 2 2 Per phase voltage 995 106 1000 volts E E      Line voltage 3 995 1723.4 volts   
  • 36. DEPT. OF ELECTRICAL ENGINEERING, COLLEGE OF ENGINEERING TRIVANDRUM 36 Thank You