TRANSFORMER
description
Transcript of TRANSFORMER
TRANSFORMER
C
vp
ip
P
Np
= Npip/S …….(1)where S is the reluctance
A transformer consists of a core made of laminated iron separated by insulators and a coil of Np turns wound around the core. This coil is supplied with an a.c voltage supply vp which then produces a current ip. Due to this current , a flux is produced which is given by an equation
dt
dN pp
v
)(dt
dNp
2p
p iv
Since current varied with time , also varied with time. A back electromagnetic force (e.m.f) will be produced which is given by the equation.
Substitute = Npip/S into the above equation , then
……(2)
……(3)
dt
2sindNpp
ftv m
= m sin 2ft
If ip is sinusoidal, the flux produced also sinusoidal, i.e
therefore
vp = NP2fmcos 2ft = NP2fmsin (2ft + /2)
The peak value = Vpm = NP2fm
and vp is leading the flux by /2.
mmpm
p f44.4πf2707.02
VV PP NNThe rms value
……(4)
……(5)
……(6)
……(7)
dt
dNss
v ……(8)
C
vp
ip
vs
is
LoadP S
N
s
N
p
primary secondary
When another coil is wound on the other side of the core with no of turns Ns , then the fux will induce the e.m.f vS as given by
From (2) and (8) we get
p
s
p
s
N
N
V
V
…….(9)
p
s
p
s
N
N
v
v
Or in rms value
With load , is will flow in the load, mmf at load will equal to the mmf at input, then (in rms value)
NpIp = NsIs
rearrange
p
s
s
p
N
N
I
I
…….(10)
…….(12)
…….(11)
For ideal transformer, the energy transferred will be the same as input. Thus power at primary is same power at secondary.
Pp = Ps
or IpVp = IsVs
NP : NS
VP VS
Primary Secondary
Symbol for ideal transformer
A 250 kVA,11000V/400V, 50Hz single –phase transformer has 80 turns on the secondary. Calculate(a) The appropriate values of the primary and secondary currents;(b) The approximate number of primary turns;(c) the maximum value of the flux.
(a) Full-load primary current
AI s 625400
10250
V
P -3
s
AV
PI
pp 7.22
11000
10250 3
Full-load secondary current
220011000400
80V
V
NN P
s
sP
p
s
p
s
N
N
V
V
mf N44.4E
mWbfm 5.22
508044.4
400
N4.44
E
s
s
(b) Number of primary turns
recall
(c) Maximum flux
recall
EP VP VSNSNP
IO
Ideal transformer with no load
Io is the no load current when the secondary is open
circuit. This current consists of Iom that is required to
produce the flux in the core (it is in phase) and Io1 is to
compensate the hysteresis and eddy current losses.
VP= emf of supply to the primary coil
and 90o leads the flux.
EP=emf induced in the primary coil and
same phase as VP.
VS=emf induced in the secondary coil
and 90o lags the flux.
Iom=magnetizing current to produce flux
and it is in phase with flux.
Io1=current to compensate the losses due
to hysteresis and eddy current.
Io=the no load current and given by
21
2I oomo II
o
oo I
I 1cos Power factor
Phasor diagram for no load transfomer
IOm
IOI
EP
VP
IO
VS
Transformer 1 Transformer 2
Low voltage generator
Low voltage load
High voltage line
Transformer converts the energy to high electrical voltage and transmits in the high voltage line. At the load, the high voltage energy is converted to low voltage. In this way, it will compensate the losses during transferring of the voltage energy.
A single-phase transformer has 480 turns on the primary and 90 turns on the secondary. The mean length of the flux path in core is 1.8m and the joints are equivalent to the airgap of 0.1mm. The value of the magnetic field strength for 1.1 T in the core is 400A/m, the corresponding core loss is 1.7W/kg at 50Hz and the density of the core is 7800kg/m3.If the maximum value of the flux is to be 1.1T when a p.d of 2200V at 50Hz is applied to the primary, calculate:(a) the cross-sectional area of the core;(b) the secondary voltage on no load;(c) the primary current and power factor on no load
AB
recall mf N44.4E
Wbfm 0206.0
5048044.4
2200
4.44N
E
p
p
20187.01.1
026.0A m
Bm
recall
(a)
(b)p
s
p
s
N
N
V
Vrecal
l
V4132200480
90V
V
NN P
s
sP
Practically 10% more allow for insulator
AC 7208.1400HC
AB
ao
aa 5.870001.0104
1.1H
7
A5.8075.87720
AN
HIom 682.1
480
5.807
INH
AIomom 19.1682.1707.0707.0I
(c) magnetomotive force (mmf) for the core is
mmf for the airgap is
Total mmf is
Maximum magnetizing current
recall
Rms value
30337.00187.08.1 mA
kgdensityVol 26378000337.0.
W4477.1263
AV
PI
po 203.0
2200
4471
laggingI
I
o
168.021.1
203.0cos 01
AIII oomo 21.1203.019.1 2221
2
Volume of core
mass of core
Core loss= loss rate x mass
Core-loss component of current
No load current
Power factor
E1 V1 V2
I1 I2
L(2)
Loaded transformer
L(2)= load with power factor of cos 2
V1 = emf at supply
E1=induced voltage at primary
V2=emf at load
E2=induced voltage at secondary
I1= primary current
I2=secondary current
Phasor diagram
Io
V 1 , E 1
- I 2 I 1
2
1
O
V 2 , E 2
I2
‘
A single-phase transformer has 1000 turns on the primary and 200 turns on the secondary. The no load current is 3A at a power factor 0.2 lagging when secondary current is 280A at a power factor of 0.8 lagging. Calculate the primary current and the power factor. Assume the voltage drop in the windings to be negligible.
A562801000
200I
N
NI S
P
SP
Recall Equation 12p
s
s
p
N
N
I
I
therefore
ooIII sinsinsin '2'211
ooIII coscoscos '2'211
6.0sin '2
98.0sin o2.0c oos
8.0c '2 os
A4.452.038.056
'50381o
AI 3.5854.364.45 221
laggingos o 78.050'38cosc 1
805.04.45
54.36tan 1
A54.3698.036.056
Io
V 1 , E 1
- I 2 I 1
2
1
O
V 2 , E 2
I2
‘
Solve for horizontal and vertical components
Power factor
Path of leakage
V2’
R1 L1 L2 R2
RCLm V2E1
I1’I1
Equivalent circuit of transformer
Flux leakage is due to secondary current that produce flux which encounter the primary flux. Some of the flux will link to its own windings and produce induction. This is represented by inductance L1. Similarly with the flux in secondary and represented by L2.
There are four main losses•Dissipated power by wire resistance of the windings (I2R)•Power due to hysteresis•Power due to eddy current•Power via flux leakages.
R1= wire resistance of primary windingsL1=inductance due to leakage flux in primary windingsRC=resistance represent power loss due to in hysteresis and eddy currentLm= inductance due to magnetizing current Iom
L2=inductance due to leakage flux in secondary windingsR2=wire resistance of secondary windings
E2
R1 L1 L2 R2
RCLm V2V1
I1’I1
Equivalent circuit of transformer
E1
Phasor diagram for a transformer on load
V1
E1
I2
-I2’
I1X1
V2
E2
I1
I0
I1R1
I1Z1
I2X2
I2Z2
I2R2
1
2
2
2
12
2
2
12'2
V
VX
N
NXX
2
2
12
2
1
22'2
V
VR
I
IRR
222'2
21 RIRI
We can replace R2 by inserting R2’ in the primary thus the equivalent resistance is
Giving us
Similarly
2
2
121'21
V
VRRRRRe
22eee XRZ
e
e
R
Xtan e
eee ZX sin
eee ZR cos
then
and
where
2
2
121'21
V
VXXXXX e
(b)
Transformer simplified circuit
Ze
V1 E1=V2’
I1 I2
To loadE2=V2
Phasor diagram of simplified equivalent circuit of transformer
I1R e
I1Z e
I1X e e
Magnified Ze portion
I1X e
I1
E 1=V 2'
V 1
I1Z e
I1R e
E 2 ,V 2
I2
e
Complete
o-2
voltageload-no
voltageload-fullvoltageload-noregulationVoltage
1
212 N
NVV
p
s
p
s
N
N
V
Vrecall
Secondary voltage on no-load
V2 is a secondary terminal voltage on full load
1
21
21
21
regulationVoltage
NN
V
VNN
VSubstitute we have
1
221 sincos
V
XRIregulationvoltageunitPer ee
centperV
NN
VV
1001
2
121
unitperV
NN
VV
1
2
121
regulationVoltage
Or
From phasor diagram can be proved that
1
21 cos
V
ZIregulationvoltageunitPer ee
Or
A 100kVA transformer has 400 turns on the primary and 800 turns on the secondary. The primary and secondary resistances are 0.3 and 0.01 respectively, and the corresponding leakage reactances are 1.1and 0.035 respectively. The supply voltage is 2200V. Calculate:
(a)The equivalent impedance referred to the primary circuit;(b)The voltage regulation and the secondary terminal voltage for
full load having a power factor of (i) 0.8 lagging and (ii) 0.8 leading.
(c)The percentage resistance and leakage reactance drops of the transformer
AV
PcurrentprimaryloadFull 45.45
2200
10100 3
unitper0336.0
2200
6.0975.18.055.045.45
975.1
80
400035.01.1
22
2
121 V
VXXX e
05.2975.155.0 2222eee XRZ
55.0
80
40001.03.0
22
2
121 V
VRRRe
(a)
(b) (i)
1
221 sincos
V
XRIregulationvoltageunitPer ee
centper36.3
V78.44678.6440
VN
NV
P
SP 440
400
802200
centper54.1
(b) (ii) power factor 0.8 leading
unitperregulationVoltage 0154.0
2200
6.0975.18.055.045.45
V8.140336.0440
V78.60154.0440
Sec. terminal voltage on no-load
The decreasing of full-load voltage is
V2.4258.14440 Therefore the secondary full-load voltage
The increasing of full-load voltage is
Therefore the secondary full-load voltage
1
e1
V
RI
2200
55.045.45 0.0114
0.0114%
Per unit
ltageprimary vo
primary toreferred
resistance equivalent
currentprimary
load-full
unitper drop Resistance
load-noon voltagesecondary
secondary toreferred
resistance equivalent
currentsecondary
load-full
unitper drop ResistanceOr
drop Resistance
Alternative
Full load secondary current
Recall Equation 12p
s
s
p
N
N
I
I
Equivalent resistance referred to secondary
AS 2.22745.4580
400I
N
NI P
S
P
022.0
400
803.001.0
22
1
212 N
NRRRe
VN
NV
P
SP 440
400
802200 Secondary voltage on no-load
440
022.02.227
load-noon voltagesecondary
secondary toreferred
resistance equivalent
currentsecondary
load-full
unitper drop Resistance
1.14% unit per 0.0114
2200
975.145.45
ltageprimary vo
primary toreferred
resistance leakage equivalent
currentprimary
load-full
unitper drop ractance Leakage
975.1
80
400035.01.1
22
2
121 V
VXXX e
%08.4unitper 0408.0
primary toreferred resistance leakage equivalent
AV
PcurrentprimaryloadFull 45.45
2200
10100 3