Chapter 12 Three-Phase Circuits. Power Factor Correction A balanced three-phase circuit Medium...
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Transcript of Chapter 12 Three-Phase Circuits. Power Factor Correction A balanced three-phase circuit Medium...
Chapter 12
Three-Phase Circuits
Power Factor Correction
A balanced three-phase circuit
Medium Voltage Metal Enclosed Capacitor Banks
Three-Phase Voltages
(b) Balanced three-phase voltages
(a) The three windings on a cylindrical drum used to obtain three-phase voltages
2 cos
2 cos( 120 )
2 cos( 240 )
aa
bb
cc
v V t
v V t
v V t
Three-Phase Voltages
Generator with six terminals
Three-Phase Balanced Voltages
0
120
240 120
aa
bb
cc
V
V
V V
V
V
V
Phase sequence or phase rotation is abcPositive Phase Sequence
0
120
240 120
a
c
b
V
V
V V
V
V
V
Phase sequence or phase rotation is acbNegative Phase Sequence
neutral terminal
(a) Y-connected sources (b) -connected sources
Two Common Methods of Connection
phase voltage
Phase and Line Voltages
The line-to-line voltage Vab of the Y-connected source
0 120
( 0.5 0.866)
3 30
ab a b
p p
p p
p
V V
V V j
V
V V V
Similarly
3 90
3 210
bc p
ca p
V
V
V
V
The Y-to-Y Circuit
A four-wire Y-to-Y circuit
The Y-to-Y Circuit (cont.)
, , anda b caA bB cC
A B C
V V V
I I IZ Z Z
nN aA bB cC I I I I
The average power delivered by the three-phase sourceto the three-phase load
A B CP P P P When ZA = ZB = ZC the load is said to be balanced
0 120 120, , and
, ( 120 ), and ( 120 )
a b caA bB cC
A B C
aA bB cC
V V V
Z Z Z
V V V
Z Z Z
V V VI I I
Z Z Z
I I I
Four - wire
0nN aA bB cC I I I I
The Y-to-Y Circuit(cont.)
2
cos( ) cos( ) cos( )
3 cos( )
A B CP P P P
V V VV V VZ Z Z
V
Z
The average power delivered to the load is
There is no current in the wire connecting the neutral nodeof the source to the neutral node of the load.
The Y-to-Y Circuit (cont.)
A three-wire Y-to-Y circuit
Three - wire We need to solve for VNn
The Y-to-Y Circuit (cont.)
0
0 120 120
a Nn b Nn c Nn
A B C
Nn Nn Nn
A B C
V V V
V V V V V V
Z Z Z
V V V
Z Z Z
Solve for VNn
( 120 ) 120 0A C A B B CNn
A C A B B C
V V V
Z Z Z Z Z Z
VZ Z Z Z Z Z
, , anda Nn b Nn c NnaA bB cC
A B C
V V V V V VI I I
Z Z Z
When the circuit is balanced i.e. ZA = ZB = ZC
The Y-to-Y Circuit (cont.)
( 120 ) 120 0
0
Nn
V V V
ZZ ZZ ZZV
ZZ ZZ ZZ
The average power delivered to the load is
2
3 cos( )
A B CP P P P
V
Z
A three-wire Y-to-Y circuit with line impedances
The Y-to-Y Circuit (cont.)
Transmission lines
The Y-to-Y Circuit (cont.)
The analysis of balanced Y-Y circuits is simpler than theanalysis of unbalanced Y-Y circuits.
VNn = 0. It is not necessary to solve for VNn . The line currents have equal magnitudes and
differ in phase by 120 degree. Equal power is absorbed by each impedance.
Per-phase equivalent circuit
Example 12.4-1 S = ?rms
rms
rms
110 0 V
110 120 V
110 120 V
a
b
c
V
V
V
50 80
50
100 25
A
B
C
j
j
j
Z
Z
Z
Unbalanced 4-wire
rms
rms
rms
110 01.16 58 A
50 80
110 1202.2 150 A
50
110 1201.07 106 A
100 25
aaA
A
bbB
B
ccC
C
j
j
j
VI
Z
VI
Z
VI
Z
Example 12.4-1 (cont.)*
*
*
68 109 VA
242 VA
114 28 VA
A aA a
B bB b
C cC c
j
j
j
S I V
S I V
S I V
The total complex power delivered to the three-phase loadis
182 379 VAA B C j S S S S
Example 12.4-2 S = ?
rms
rms
rms
110 0 V
110 120 V
110 120 V
a
b
c
V
V
V
50 80
50 80
50 80
A
B
C
j
j
j
Z
Z
Z
Balanced 4-wire
rms
110 01.16 58 A
50 80a
aAA j
V
IZ
* 68 109 VAA aA a j S I V
The total complex power delivered to the three-phase loadis
3 204 326 VAA j S S
Alsorms rms1.16 177 A , 1.16 62 AbB cC I I
68 109 VAB Cj S S
Example 12.4-3 S = ?
rms
rms
rms
110 0 V
110 120 V
110 120 V
a
b
c
V
V
V
50 80
50
100 25
A
B
C
j
j
j
Z
Z
ZUnbalanced 3-wire
Determine VNn
rms
(110 120 ) 110 120 110 0
56 151 V
A C A B B CNn
A C A B B C
Z Z Z Z Z ZV
Z Z Z Z Z Z
, , anda Nn b Nn c NnaA bB cC
A B C
V V V V V VI I I
Z Z Z
Example 12.4-3 (cont.)
1.71 48 , 2.45 3 , and 1.19 79aA bB cC I I I
* *
* *
* *
( ) 146 234 VA
( ) 94 VA
( ) 141 35 VA
A aA a aA aA A
B bB b bB bB B
C cC c cC cC C
j
j
j
S I V I I Z
S I V I I Z
S I V I I Z
The total complex power delivered to the three-phase loadis
287 364 VAA B C j S S S S
Example 12.4-4 S = ? Balanced 3-wire
rms
rms
rms
110 0 V
110 120 V
110 120 V
a
b
c
V
V
V
50 80
50 80
50 80
A
B
C
j
j
j
Z
Z
Z
rms
110 01.16 58 A
50 80a
aAA j
V
IZ
* 68 109 VAA aA a j S I V
The total complex power delivered to the three-phase loadis
3 204 326 VAA j S S
Example 12.4-5 PLoad = ? PLine = ? PSource = ?
Balanced 3-wire
per-phase equivalent circuit
100 0( ) 1.894 18.7 A
50 (377)(0.045)a
aAA j
V
IZ
The phase voltage at the load is
( ) (40 (377)(0.04)) ( ) 81 2 VAN aAj V I
Example 12.4-5 (cont.)
The power delivered by the source is
cos( )2
(100)(1.894)cos(18.7 ) 89.7 W
2
m ma V I
V IP
The power delivered to the load is2 2(1.894)
Re( ) 40 71.7 W2 2m
A A
IP Z
The power lost in the line is2 2(1.894)
Re( ) 10 17.9 W2 2m
aA Line
IP Z
Line loss 20%
The -Connected Source and Load
rms
rms
rms
120 0 V
120.1 121 V
120.2 121 V
ab
bc
ca
V
V
V
( )3.75 A
1ab bc ca
V V V
I
Total resistance around the loop
Circulatingcurrent Unacceptable
Therefore the sources connection is seldom used in practice.
The -Y and Y- Transformation
AZ BZ
CZ
1Z
3Z
2Z
1 3
1 2 3
2 3
1 2 3
1 2
1 2 3
A
B
C
Z Z
Z Z Z
Z Z
Z Z Z
Z Z
Z Z
Z
ZZ
Z
1
2
3
A B B C A C
B
A B B C A C
A
A B B C A C
C
Z Z Z Z Z Z
Z
Z Z Z Z Z Z
Z
Z
Z
ZZ Z Z Z Z Z
Z
Example
The Y- Circuits
aA AB CA
bB BC AB
cC CA BC
I I I
I I I
I I I
where
3
1
2
ABAB
BCBC
CACA
VI
Z
VI
Z
VI
Z
The Y- Circuits (cont.)
cos sin cos( 120 ) sin( 120 )
3 ( 30 )
aA AB CA
I j I j
I
I I I
or
3 3aA L pI I I I
Example 12.6-1 IP = ? IL = ?
rms
rms
rms
22030 V
3220
150 V3
22090 V
3
a
b
c
V
V
V
The -connected load is balanced with 10 50 Z
rms
rms
rms
220 0 V
220 120 V
220 240 V
AB a b
BC b c
CA c a
V V V
V V V
V V V
rms
rms
rms
22 50 A
22 70 A
22 190 A
ABAB
BCBC
CACA
VI
Z
VI
Z
VI
Z
The line currents are
22 3 20 , 22 3 100 , 22 3 220aA AB CA bB cC I I I I I
The Balanced Three-Phase Circuits
3Y
ZZ
per-phase equivalent circuit
Y-to- circuit equivalent Y-to-Y circuit
Example 12.7-1 IP = ?
rms
rms
rms
110 0 V
110 120 V
110 120 V
a
b
c
V
V
V
10 5
75 225L j
j
Z
Z25 75
3Y j Z
Z
rms1.26 66 AaaA
L Y
V
IZ Z
Example 12.7-1 (cont.)
rms rms1.26 186 A and 1.26 54 AbB cC I I
rms
rms
rms
99.6 5 V
99.6 115 V
99.6 125 V
AN aA Y
BN
CN
V I Z
V
V
The voltages in the per-phase equivalent circuit are
rms
rms
rms
172 35 V
172 85 V
172 155 V
AB AN BN
BC BN CN
CA CN AN
V V V
V V V
V V V
The line-to-line voltages arerms
rms
rms
0.727 36 A
0.727 156 A
0.727 84 A
ABAB
BCBC
CACA
VI
Z
VI
Z
VI
Z
Instantaneous and Average Power in BTP Circuits
One advantage of three-phase power is the smooth flow ofenergy to the load.
2 2 2
2
2 2
2
( )
1 cos2 1 cos2( 120 ) 1 cos2( 240 )2
3cos2 cos(2 240 )cos(2 480 )
2 20
3
2
ab bc cav v vp t
R R R
Vt t t
R
V Vt t t
R R
V
R
2
cos , cos( 120 ),
and cos( 240 )
(1 cos2 )cos
2
ab bc
ca
v V t v V t
v V t
tt
The instantaneous power
Instantaneous and Average Power in BTP Circuits
The total average power delivered to the balanced Y-connected load is
33cos()
3cos()
3cos()3
3cos()
YAPLAVAI
PL
LL
LL
PPVI
VI
VI
VI
,aA L AI AN P AVI V I V Phase A
Instantaneous and Average Power in BTP Circuits
The total average power delivered to the balanced -connected load is
33cos()
3(3)cos()3
3cos()
ABABAB
LP
PL
PPVI
IV
VI
Example 12.8-1 P = ?
rms
rms
rms
110 0 V
110 120 V
110 120 V
a
b
c
V
V
V
10 5
75 225L j
j
Z
Z
rms1.26 66 AaaA
L Y
V
IZ Z
rms99.6 5 VAN aA Y V I Z
3(99.6)(1.26)cos(5 ( 66 )) 122.6 WP
Two-Wattmeter Power Measurement
cc = current coilvc = voltage coil
W1 read
1 1cosAB AP V I
W2 read
2 2cosCB CP V I
For balanced load with abc phase sequence
1 230 and 30a a
is the angle between phase current and phase voltage of phase a a
Two-Wattmeter Power Measurement(cont.)
1 2
2 cos cos30
3 cos
L L
L L
P P P
V I
V I
To determine the power factor angle
1 2 2cos cos30L LP P V I
1 2 ( 2sin sin 30 )L LP P V I
1 2
1 2
2cos cos30 3
( 2sin sin 30 ) tanL L
L L
P P V I
P P V I
11 2 1 2
1 2 1 2
tan 3 or tan 3P P P P
P P P P
Example 12.9-1 P = ?
10 45 Z
line-to-line voltage = 220Vrms
The phase voltage220
303
A V
The line current220 30
12.7 7510 3 45
AA
V
IZ
and 12.7 195B I
1 1
2 2
cos 2698 W
cos 723 WAC A
BC B
P V I
P V I
1 2 3421 WP P P
Electrodynamic Wattmeter
Digital Power Meter VAR Meter
pf Meter
Summary
Three-Phase voltages
The Y-to-Y Circuits
The -Connected Source and Load
The Y-to- Circuits
Balanced Three-Phase Circuits
Instantaneous and Average Power in Bal. 3 Load
Two-Wattmeter Power Measurement