Bài giảng Power Circuits and Electromechanics - Lecture 2 - Nguyễn Quang Nam

ECE430  
Power Circuits and Electromechanics  
Dr. Nam Nguyen-Quang  
Fall 2009  
Lecture 2  
1
Three-phase systems  
Voltage in each phase differ from the other phases by 1200. In  
positive (also a-b-c) phase sequence, the three voltages are given by  
t 1200  
vcc' Vm cos  
t 1200  
vaa' Vm cos
t
  
vbb' Vm cos  
Three-phase connections: wye connection and delta connection  
In wye connection, terminals a’, b’, and c’ are joined and labeled as  
neutral terminal n.  
a
ia  
+
ia, ib, and ic are line currents, which are  
also equal to the phase currents. in is  
neutral line current.  
n
in  
ib  
c
b
ic  
Lecture 2  
2
1
Three-phase systems (cont.)  
In delta connection, terminals a’ is connected to b, and b’ to c. Because  
vac’ = vaa’(t) + vbb’(t) + vcc’(t) = 0, as can be verified mathematically, c’ is  
finally connected to a.  
ia  
c’ a  
Line and phase quantities  
Since both supply and load can be wye or  
delta connected, there are 4 possible  
combinations: wye-wye, wye-delta, delta-  
wye, and delta-delta (supply-load).  
ib  
ic  
a’  
c
b’  
b
• wye-wye connection, balanced condition:  
Van V00  
Vbn V 1200  
Vcn V1200  
Lecture 2  
3
Three-phase systems (cont.)  
where Vis the rms value of phase-to-neutral voltage.  
The line-to-line voltages are given by  
Vca Vcn Van  
Vab Van Vbn  
Vbc Vbn Vcn  
V
For example, magnitude of ab can be calculated as  
Vab 2Vcos  
300  
3V  
Vcn  
Vab  
Vca  
From the phasor diagram, it can be seen  
Van  
Vab 3V300  
Vca 3V1500  
Vbc 3V  900  
Vbn  
Vbc  
Under balanced condition, in = 0 (no neutral current)  
Lecture 2  
4
2
Three-phase systems (cont.)  
• wye-delta connection, balanced condition:  
Without losing generality, assuming line-to-line voltages are  
Vab VL00  
Vbc VL1200  
Vca VL1200  
Phase currents I1, I2, and I3 in the three legs of  
delta-connected load lag the respective  
Vca  
I3  
voltages by , and have the same magnitude of  
I. It can be seen from the phasor diagram  
Vab  
I2  
I1  
Ia  
3I  300  
Ib 3I 1500   
Ic 3I900  
Ia  
Vbc  
Wye connection: V 3V and I I , delta connection:  
VL V  
L
L
and  
IL 3I  
Lecture 2  
5
Power in balanced three-phase circuits  
Balanced Y-connected load  
In a balanced system, the magnitudes of voltages in all phases are the  
same, and so also the current magnitudes. Let these be Vand I. The  
power per phase is then  
P VIcos  
  
Total power is  
   
   
P 3P 3VIcos 3VL IL cos   
T
SVI* VI  
Complex power per phase is  
And total complex power is  
ST 3S3VI3VL IL  
Note that is the phase angle between the phase voltage and phase current  
Lecture 2  
6
3
Power in balanced three-phase circuits (cont.)  
Balanced -connected load  
Similar to the case of balanced Y-connected load, per phase and total  
power can be calculated using the same formulae.  
It can be seen that for a balanced load, the expression for total complex  
power is the same both for wye and delta connections, provided line-to-  
line voltages and line currents are used.  
Hence, calculations can be done on a three-phase or per-phase basis.  
Ex. 2.12 and 2.13: see text book  
Lecture 2  
7
Per-phase equivalents  
-Y conversion  
Given a delta-connected load where impedance of each phase is Z, the  
equivalent wye circuit has a phase impedance of ZY = Z/3. This can be  
proved by equating the impedance across 2 arbitrary lines in both cases.  
Instead of analyzing the delta circuit, the per-phase equivalent circuit can be  
used after doing the -Y conversion.  
Ex. 2.14: Draw the per-phase equivalent circuit for a given circuit.  
Replace -connected capacitor bank by a Y-connected bank with phase  
impedance of –j15/3 = -j5 . The resulting wye-connected circuit can then be  
simplified to give the per-phase equivalent circuit.  
Lecture 2  
8
4
Class examples  
Ex. 2.15: 10 induction motors in parallel, find three-phase kVAR  
rating of a capacitor bank to improve overall PF to unity?  
Per-phase real power is 30 x 10 / 3 = 100 kW, at lagging PF = 0.6. Per-  
phase kVA is therefore 100/0.6. Hence,  
100103  
SScos1  
0.6  
0.6 j0.8 VA 100 j133.33 kVA  
0.6  
A capacitor bank can be connected in parallel to the load for improving  
overall PF. The capacitor bank needs to supply all the reactive power to  
bring PF to unity. This means per-phase Qcap = 133.33 kVAR, and three-  
phase kVAR required will be 3(133.33) = 400 kVAR.  
Lecture 2  
9
Class examples  
Ex. 2.16: Suppose in Ex. 2.15, the new PF is to be 0.9 lagging, what  
is the kVAR needed?  
S100 j133.33 kVA  
New PF is 0.9 lagging, therefore new per-phase reactive power is  
2
2
Qnew P 1 PF 1 100 1 0.9 1 48.43kVAR  
133.33  
kVAR  
The capacitor bank therefore needs to supply  
133.33 + 48.43 = 84.9 kVAR, and three-phase  
kVAR required will be 3(84.9) = 254.7 kVAR.  
48.43  
kVAR  
Ex. 2.17: see text book  
100 kW  
Lecture 2  
10  
5
In class quiz  
Problem 2.21: A three-phase load of 15 kVA with a PF of 0.8  
lagging is connected in parallel with a three-phase load of 36  
kW at 0.6 PF leading. The line-to-line voltage is 2000 V.  
a) Find the total complex power and power factor  
b) How much kVAR is needed to make the PF unity?  
Special question: A three-phase wye-connected load with a  
unity PF is being supplied from a three-phase power system.  
How does the load power change if the load is now rewired in  
delta configuration?  
Lecture 2  
11  
6
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