TRANSFORMERS
Introduction
Introduction
• A transformer is a static machines
static machines.
• The word ‘transformer’ comes form the word ‘transform’.
The word ‘transformer’ comes form the word ‘transform’.
• Transformer is not an energy conversion device
not an energy conversion device, but is a device that
device that
changes AC electrical power at one voltage level into AC electrical
changes AC electrical power at one voltage level into AC electrical
power at another voltage level through the action of magnetic field,
power at another voltage level through the action of magnetic field,
without a change in frequency.
without a change in frequency.
• It can be either to step-up or step down.
It can be either to step-up or step down.
Generation
Generation
Station
Station
TX1 TX1
Distribution
Distribution
s
s TX1
TX1
T
Transmission
ransmission
System
System
33/13.5k
33/13.5k
V
V
13.5/6.6kV
13.5/6.6kV
6.6kV/
6.6kV/
415V
415V
Transformer Construction
• Two types of iron-core construction:
a) Core - type construction
b) Shell - type construction
• Core - type construction
Transformer Construction
• Shell - type construction
Ideal Transformer
• An ideal transformer is a transformer which has no loses
which has no loses,
i.e. it’s winding has no ohmic resistance, no magnetic
leakage, and therefore no I2
R and core loses.
• However, it is impossible
impossible to realize such a transformer in
practice.
• Yet, the approximate characteristic of ideal transformer
approximate characteristic of ideal transformer
will be used in characterized the practical transformer.
will be used in characterized the practical transformer.
V
V1
1 V
V2
2
N
N1
1 : N
: N2
2
E
E1
1 E
E2
2
I
I1
1 I
I2
2
V1 – Primary Voltage
V1 – Primary Voltage
V2 – Secondary Voltage
V2 – Secondary Voltage
E1 – Primary induced Voltage
E1 – Primary induced Voltage
E2 – secondary induced Voltage
E2 – secondary induced Voltage
N1:N2 – Transformer ratio
N1:N2 – Transformer ratio
Transformer Equation
• Faraday’s Law states that,
– If the flux passes through a coil of wire, a voltage will be
induced in the turns of wire. This voltage is directly
proportional to the rate of change in the flux with respect
of time.
If we have N
N turns of wire,
dt
t
d
Emf
V ind
ind
)
(




dt
t
d
N
Emf
V ind
ind
)
(




Lenz’s Law
Transformer Equation
• For an ac sources,
– Let V(t) = Vm sint
i(t) = im sint
Since the flux is a sinusoidal function;
Then:
Therefore:
Thus:
t
t m 
sin
)
( 


t
N
dt
t
d
N
Emf
V
m
m
ind
ind



cos
sin







m
m
ind
ind fN
N
Emf
V 



 
 2
(max)
m
m
m
rms
ind fN
fN
N
Emf 




 44
.
4
2
2
2
)
(


Transformer Equation
• For an ideal transformer
• In the equilibrium condition, both the input power will be equaled to the
output power, and this condition is said to ideal condition of a
transformer.
• From the ideal transformer circuit, note that,
m
m
fN
E
fN
E




2
2
1
1
44
.
4
44
.
4
1
2
2
1
2
2
1
1 cos
cos
I
I
V
V
I
V
I
V
power
output
power
Input






………………… (i)
2
2
1
1 V
E
and
V
E 

Transformer Equation
a
I
I
N
N
E
E
Therefore 


1
2
2
1
2
1
,
Where, ‘a
a’ is the Voltage Transformation Ratio
Voltage Transformation Ratio; which will
determine whether the transformer is going to be step-up
or step-down
E
E1
1 > E
> E2
2
For a >1
For a >1
For a <1
For a <1 E
E1
1 < E
< E2
2
Transformer Rating
• Transformer rating is normally written
written in terms of
Apparent Power
Apparent Power.
• Apparent power is actually the product of its rated
its rated
current and rated voltage
current and rated voltage.
2
2
1
1 I
V
I
V
VA 

 Where,
 I1 and I2 = rated current on primary and secondary winding.
 V1 and V2 = rated voltage on primary and secondary winding.
 Rated currents are actually the
Rated currents are actually the full load currents
full load currents in
in
transformer
transformer
Example
1. 1.5kVA single phase transformer has rated voltage of
144/240 V. Finds its full load current.
Solution
Solution
A
I
A
I
FL
FL
6
240
1500
45
.
10
144
1500
2
1




Practical Transformer (Equivalent
Circuit)
V1 = primary supply voltage
V2 = 2nd
terminal (load) voltage
E1 = primary winding voltage
E2 = 2nd
winding voltage
I1 = primary supply current
I2 = 2nd
winding current
I1
’
= primary winding current
Io = no load current
V1 = primary supply voltage
V2 = 2nd
terminal (load) voltage
E1 = primary winding voltage
E2 = 2nd
winding voltage
I1 = primary supply current
I2 = 2nd
winding current
I1
’
= primary winding current
Io = no load current
V
V1
1
I
I1
1 R
R1
1
X
X1
1
R
RC
C
I
Ic
c
X
Xm
m
I
Im
m
I
Io
o
E
E1
1 E
E2
2
V
V2
2
I
I1
1
’
’
N
N1
1: N
: N2
2
R
R2
2
X
X2
2
Load
Load
I
I2
2
Single Phase Transformer (Referred to
Primary)
Actual Method
Actual Method
2
2
2
2
2
2
1
2 '
' X
a
X
OR
X
N
N
X 









2
2
2
2
2
2
1
2 '
' R
a
R
OR
R
N
N
R 









V
V1
1
I
I1
1 R
R1
1 X
X1
1
R
RC
C
I
Ic
c
X
Xm
m
I
Im
m
I
Io
o
E
E1
1 E
E2
2 V
V2
2
I
I2
2
’
’ N
N1
1: N
: N2
2
R
R2
2
’
’ X
X2
2
’
’
Load
I
I2
2
a
I
I
aV
V
OR
V
N
N
V
E
2
2
2
2
2
2
1
'
2
1
'
'












Single Phase Transformer (Referred to
Primary )
)
Approximate Method
Approximate Method
2
2
2
2
2
2
1
2 '
' R
a
R
OR
R
N
N
R 









2
2
2
2
2
2
1
2 '
' X
a
X
OR
X
N
N
X 









V
V1
1
I
I1
1 R
R1
1
X
X1
1
R
RC
C
I
Ic
c
X
Xm
m
I
Im
m
I
Io
o
E
E1
1 E
E2
2 V
V2
2
I
I2
2
’
’ N
N1
1: N
: N2
2
R
R2
2
’
’
X
X2
2
’
’
Load
I
I2
2
a
I
I
aV
V
OR
V
N
N
V
E
2
2
2
2
2
2
1
'
2
1
'
'












Example Problem
1. A 10 kVA single phase transformer 2000/440V has
primary resistance and reactance of 5.5 and 12
respectively, while the resistance and reactance of
secondary winding is 0.2 and 0.45  respectively.
Calculate:
i. The parameter referred to high voltage side and
draw the equivalent circuit
ii. The approximate value of secondary voltage at full
load of 0.8 lagging power factor, when primary
supply is 2000V
Example 1 (Cont)
Solution
Solution
R1=5.5 , X1=j12 
R2=0.2 , X2=j0.45 
i) Refer to H.V side (primary)
R2’=(4.55)2
(0.2) = 4.14,
X2’=j(4.55)2
0.45 = j9.32 
Therefore,
R01=R1+R2’=5.5 + 4.13 = 9.64 
X01=X1+X2’=j12 + j9. 32 = j21.32 
V1 aV2
R01 X01
21.32
9.64
I1
Example 1 (Cont)
A
V
VA
IFL 5
2000
10
10 3
1



Solution
Solution
ii) Secondary voltage
p.f = 0.8
Cos  = 0.8
 =36.87o
Full load,
From eqn
o
o
o
o
o
V
V
j
aV
I
jX
R
V
8
.
0
6
.
422
)
55
.
4
(
)
87
.
36
5
)(
32
.
21
64
.
9
(
0
2000
)
)(
(
0
2
2
2
1
01
01
1













 
Transformer Losses
• Generally, there are two types of losses;
i.
i. Iron losses
Iron losses :- occur in core parameters
ii.
ii. Copper losses
Copper losses :- occur in winding resistance
i.
i. Iron Losses
Iron Losses
ii
ii Copper Losses
Copper Losses
circuit
open
c
c
c
iron P
R
I
P
P 

 2
)
(
02
2
2
01
2
1
2
2
2
1
2
1
)
(
)
(
,
)
(
)
(
R
I
R
I
P
referred
if
or
P
R
I
R
I
P
P
cu
circuit
short
cu
copper






Transformer Efficiency
• To check the performance of the device, by
comparing the output with respect to the input.
• The higher the efficiency, the better the system.
%
100
cos
cos
%
100
%
100
,
2
2
2
2









cu
c
losses
out
out
P
P
I
V
I
V
P
P
P
Power
Input
Power
Output
Efficiency



%
100
cos
cos
%
100
cos
cos
2
)
(
)
(








cu
c
n
load
cu
c
load
full
P
n
P
nVA
nVA
P
P
VA
VA






Where, if ½ load, hence n = ½ ,
½ load, hence n = ½ ,
¼ load, n= ¼ ,
¼ load, n= ¼ ,
90% of full load, n =0.9
90% of full load, n =0.9
Where Pcu = Psc
Pc = Poc
Voltage Regulation
• The purpose of voltage regulation is
basically to determine the percentage of
voltage drop between no load and full
load.
• Voltage Regulation can be determine
based on 3 methods:
a) Basic Defination
b) Short – circuit Test
c) Equivalent Circuit
Voltage Regulation
(Basic Definition)
• In this method, all parameter are being referred
to primary or secondary side.
• Can be represented in either
 Down – voltage Regulation
%
100
. 


NL
FL
NL
V
V
V
R
V
 Up – Voltage Regulation
%
100
. 


FL
FL
NL
V
V
V
R
V
Tap Changer
A transformer tap is a connection point
along a transformer winding that allows a
certain number of turns to be selected.
By this means, a transformer with a
variable turns ratio is produced, enabling
voltage regulation of the output. The tap
selection is made via a tap changer
mechanism.
Three Phase Transformers
 3 single phase transformers connected together
1.Star/Delta winding arrangements
2. Easy to replace failed units
 Common core device
1. Lighter and cheaper than 3 individual units
2. 6 rather than 12 external connections
3. Whole transformer must be replaced if single
winding fails .
For both cases analysis procedure identical!
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  • 1.
  • 2.
    Introduction Introduction • A transformeris a static machines static machines. • The word ‘transformer’ comes form the word ‘transform’. The word ‘transformer’ comes form the word ‘transform’. • Transformer is not an energy conversion device not an energy conversion device, but is a device that device that changes AC electrical power at one voltage level into AC electrical changes AC electrical power at one voltage level into AC electrical power at another voltage level through the action of magnetic field, power at another voltage level through the action of magnetic field, without a change in frequency. without a change in frequency. • It can be either to step-up or step down. It can be either to step-up or step down. Generation Generation Station Station TX1 TX1 Distribution Distribution s s TX1 TX1 T Transmission ransmission System System 33/13.5k 33/13.5k V V 13.5/6.6kV 13.5/6.6kV 6.6kV/ 6.6kV/ 415V 415V
  • 3.
    Transformer Construction • Twotypes of iron-core construction: a) Core - type construction b) Shell - type construction • Core - type construction
  • 4.
  • 5.
    Ideal Transformer • Anideal transformer is a transformer which has no loses which has no loses, i.e. it’s winding has no ohmic resistance, no magnetic leakage, and therefore no I2 R and core loses. • However, it is impossible impossible to realize such a transformer in practice. • Yet, the approximate characteristic of ideal transformer approximate characteristic of ideal transformer will be used in characterized the practical transformer. will be used in characterized the practical transformer. V V1 1 V V2 2 N N1 1 : N : N2 2 E E1 1 E E2 2 I I1 1 I I2 2 V1 – Primary Voltage V1 – Primary Voltage V2 – Secondary Voltage V2 – Secondary Voltage E1 – Primary induced Voltage E1 – Primary induced Voltage E2 – secondary induced Voltage E2 – secondary induced Voltage N1:N2 – Transformer ratio N1:N2 – Transformer ratio
  • 6.
    Transformer Equation • Faraday’sLaw states that, – If the flux passes through a coil of wire, a voltage will be induced in the turns of wire. This voltage is directly proportional to the rate of change in the flux with respect of time. If we have N N turns of wire, dt t d Emf V ind ind ) (     dt t d N Emf V ind ind ) (     Lenz’s Law
  • 7.
    Transformer Equation • Foran ac sources, – Let V(t) = Vm sint i(t) = im sint Since the flux is a sinusoidal function; Then: Therefore: Thus: t t m  sin ) (    t N dt t d N Emf V m m ind ind    cos sin        m m ind ind fN N Emf V        2 (max) m m m rms ind fN fN N Emf       44 . 4 2 2 2 ) (  
  • 8.
    Transformer Equation • Foran ideal transformer • In the equilibrium condition, both the input power will be equaled to the output power, and this condition is said to ideal condition of a transformer. • From the ideal transformer circuit, note that, m m fN E fN E     2 2 1 1 44 . 4 44 . 4 1 2 2 1 2 2 1 1 cos cos I I V V I V I V power output power Input       ………………… (i) 2 2 1 1 V E and V E  
  • 9.
    Transformer Equation a I I N N E E Therefore    1 2 2 1 2 1 , Where,‘a a’ is the Voltage Transformation Ratio Voltage Transformation Ratio; which will determine whether the transformer is going to be step-up or step-down E E1 1 > E > E2 2 For a >1 For a >1 For a <1 For a <1 E E1 1 < E < E2 2
  • 10.
    Transformer Rating • Transformerrating is normally written written in terms of Apparent Power Apparent Power. • Apparent power is actually the product of its rated its rated current and rated voltage current and rated voltage. 2 2 1 1 I V I V VA    Where,  I1 and I2 = rated current on primary and secondary winding.  V1 and V2 = rated voltage on primary and secondary winding.  Rated currents are actually the Rated currents are actually the full load currents full load currents in in transformer transformer
  • 11.
    Example 1. 1.5kVA singlephase transformer has rated voltage of 144/240 V. Finds its full load current. Solution Solution A I A I FL FL 6 240 1500 45 . 10 144 1500 2 1    
  • 12.
    Practical Transformer (Equivalent Circuit) V1= primary supply voltage V2 = 2nd terminal (load) voltage E1 = primary winding voltage E2 = 2nd winding voltage I1 = primary supply current I2 = 2nd winding current I1 ’ = primary winding current Io = no load current V1 = primary supply voltage V2 = 2nd terminal (load) voltage E1 = primary winding voltage E2 = 2nd winding voltage I1 = primary supply current I2 = 2nd winding current I1 ’ = primary winding current Io = no load current V V1 1 I I1 1 R R1 1 X X1 1 R RC C I Ic c X Xm m I Im m I Io o E E1 1 E E2 2 V V2 2 I I1 1 ’ ’ N N1 1: N : N2 2 R R2 2 X X2 2 Load Load I I2 2
  • 13.
    Single Phase Transformer(Referred to Primary) Actual Method Actual Method 2 2 2 2 2 2 1 2 ' ' X a X OR X N N X           2 2 2 2 2 2 1 2 ' ' R a R OR R N N R           V V1 1 I I1 1 R R1 1 X X1 1 R RC C I Ic c X Xm m I Im m I Io o E E1 1 E E2 2 V V2 2 I I2 2 ’ ’ N N1 1: N : N2 2 R R2 2 ’ ’ X X2 2 ’ ’ Load I I2 2 a I I aV V OR V N N V E 2 2 2 2 2 2 1 ' 2 1 ' '            
  • 14.
    Single Phase Transformer(Referred to Primary ) ) Approximate Method Approximate Method 2 2 2 2 2 2 1 2 ' ' R a R OR R N N R           2 2 2 2 2 2 1 2 ' ' X a X OR X N N X           V V1 1 I I1 1 R R1 1 X X1 1 R RC C I Ic c X Xm m I Im m I Io o E E1 1 E E2 2 V V2 2 I I2 2 ’ ’ N N1 1: N : N2 2 R R2 2 ’ ’ X X2 2 ’ ’ Load I I2 2 a I I aV V OR V N N V E 2 2 2 2 2 2 1 ' 2 1 ' '            
  • 15.
    Example Problem 1. A10 kVA single phase transformer 2000/440V has primary resistance and reactance of 5.5 and 12 respectively, while the resistance and reactance of secondary winding is 0.2 and 0.45  respectively. Calculate: i. The parameter referred to high voltage side and draw the equivalent circuit ii. The approximate value of secondary voltage at full load of 0.8 lagging power factor, when primary supply is 2000V
  • 16.
    Example 1 (Cont) Solution Solution R1=5.5, X1=j12  R2=0.2 , X2=j0.45  i) Refer to H.V side (primary) R2’=(4.55)2 (0.2) = 4.14, X2’=j(4.55)2 0.45 = j9.32  Therefore, R01=R1+R2’=5.5 + 4.13 = 9.64  X01=X1+X2’=j12 + j9. 32 = j21.32  V1 aV2 R01 X01 21.32 9.64 I1
  • 17.
    Example 1 (Cont) A V VA IFL5 2000 10 10 3 1    Solution Solution ii) Secondary voltage p.f = 0.8 Cos  = 0.8  =36.87o Full load, From eqn o o o o o V V j aV I jX R V 8 . 0 6 . 422 ) 55 . 4 ( ) 87 . 36 5 )( 32 . 21 64 . 9 ( 0 2000 ) )( ( 0 2 2 2 1 01 01 1               
  • 18.
    Transformer Losses • Generally,there are two types of losses; i. i. Iron losses Iron losses :- occur in core parameters ii. ii. Copper losses Copper losses :- occur in winding resistance i. i. Iron Losses Iron Losses ii ii Copper Losses Copper Losses circuit open c c c iron P R I P P    2 ) ( 02 2 2 01 2 1 2 2 2 1 2 1 ) ( ) ( , ) ( ) ( R I R I P referred if or P R I R I P P cu circuit short cu copper      
  • 19.
    Transformer Efficiency • Tocheck the performance of the device, by comparing the output with respect to the input. • The higher the efficiency, the better the system. % 100 cos cos % 100 % 100 , 2 2 2 2          cu c losses out out P P I V I V P P P Power Input Power Output Efficiency    % 100 cos cos % 100 cos cos 2 ) ( ) (         cu c n load cu c load full P n P nVA nVA P P VA VA       Where, if ½ load, hence n = ½ , ½ load, hence n = ½ , ¼ load, n= ¼ , ¼ load, n= ¼ , 90% of full load, n =0.9 90% of full load, n =0.9 Where Pcu = Psc Pc = Poc
  • 20.
    Voltage Regulation • Thepurpose of voltage regulation is basically to determine the percentage of voltage drop between no load and full load. • Voltage Regulation can be determine based on 3 methods: a) Basic Defination b) Short – circuit Test c) Equivalent Circuit
  • 21.
    Voltage Regulation (Basic Definition) •In this method, all parameter are being referred to primary or secondary side. • Can be represented in either  Down – voltage Regulation % 100 .    NL FL NL V V V R V  Up – Voltage Regulation % 100 .    FL FL NL V V V R V
  • 22.
    Tap Changer A transformertap is a connection point along a transformer winding that allows a certain number of turns to be selected. By this means, a transformer with a variable turns ratio is produced, enabling voltage regulation of the output. The tap selection is made via a tap changer mechanism.
  • 23.
    Three Phase Transformers 3 single phase transformers connected together 1.Star/Delta winding arrangements 2. Easy to replace failed units  Common core device 1. Lighter and cheaper than 3 individual units 2. 6 rather than 12 external connections 3. Whole transformer must be replaced if single winding fails . For both cases analysis procedure identical!