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6/26/2014
1
Chapter 2: Basic Principles (A review)
1
Power in single-phase AC circuits
2
instantaneous voltage
instantaneous current
instantaneous power
instantaneous power is not practical to use so let’s simplify it!
6/26/2014
2
3
Trigonometric identity
iv  
Phase angle between voltage and current
4
Average value of a signal s(t) =>

T
dtts
T 0
)(
1
T: period
Let’s first find the average value of
 
T
VIdttpR
T 0
cos)(
1
 cosVIP 
Average power
Active power
Realpower
Unit is Watts (W)
kW
MW
Since P is not zero, it is converted into other forms of energy; such as motion,heat,light,etc...
6/26/2014
3
5
Secondly let’s find the average value of
 
T
dttpX
T 0
0)(
1
Meaning of zero is that pX(t) does not do any work !
 It is the oscillating component of instantaneous power and should be considered together with
active power P
 We define reactive power Q as the amplitude of this oscillating power
Unit is volt-ampere-reactive (VAR)
kVAR
MVAR
6
BOX
i(t)
+
v(t)
For RESISTIVE component:
0 iv  No phase angle difference between voltage and current
VIVIVIP  0coscos Real power associated with R
00sinsin  VIVIQ  No reactive power associated with R
Proof ?
6/26/2014
4
7
BOX
i(t)
+
v(t)
For INDUCTIVE component:

90 iv  Phase angle difference between voltage and current
090coscos  VIVIP  No Real power associated with L
VIVIVIQ  90sinsin Reactive power associated with L
Proof ?
8
BOX
i(t)
+
v(t)
For CAPACITIVE component:

90 iv  Phase angle difference between voltage and current
0)90cos(cos  VIVIP  No Real power associated with C
VIVIVIQ  )90sin(sin Reactive power associated with C
Proof ?
What is the meaning of «-» sign ?
6/26/2014
5
9
Let’s remember BOX theory !
BOX
I
+
V ?
+
I: rms BOX current
V: rms BOX voltage
For the configuration above ( If i(t) enters to the BOX at (+) terminal)
Consumed Produced
P>0 P<0
Q>0 Q<0
In short: negative P or Q means
production or generation !
Real Power
Reactive Power
Summary
10
6/26/2014
6
11
Figure 2.1
12
Solution:
6/26/2014
7
Complex power
13
voltage and current phasors
Phasor Diagram
Complex power
Power triangle
Apparent power
Complex power balance
14
source load
PG
+ losses
QG
PL
QL
PLoss
QLoss
PG=PD=PL+Ploss
QG=QD=QL+Qloss
SG=sqrt(PG^2+QG^2)
Demand Side
SD=sqrt(PD^2+QD^2)
SG=SD
Generation Side
6/26/2014
8
15
Power factor correction
16
Lagging pf Unity pf
Power factor correction
6/26/2014
9
17
Power factor correction
18
6/26/2014
10
Complex power flow
19Bus1 Bus2
Transmission line
Sflow
Turkey power grid
20
Let’s find complex power flow from Bus1 to Bus2
Real power flow from Bus1 to Bus2
Reactive power flow from Bus1 to Bus2
6/26/2014
11
21
Which parameter(s) more or less will effect real power flow ?
Realpowerflow
Less effective
More effective
• Tight bus voltage control (around 1.0 pu)
• Voltage stability concerns
Real power can be effectively controlled/governed by angle difference
What is the maximum possible real power flow on a line?
22
Which parameter(s) will effect reactive power flow ?
Reactivepowerflow
Less effective
Voltage difference
(more effective)
• Angle difference is generally small
• Transient stability concerns
Reactive power can be effectively controlled/governed by voltage magnitude difference
6/26/2014
12
23
BALANCED THREE-PHASE CIRCUITS
24
6/26/2014
13
PHASE-SEQUENCE
25
Hint: check the 2nd phase (ph-B)
26
Y-connected Loads
• Line-to-neutral voltages
• Ref. A is chosen arbitrarily as reference
• Positive sequence
Calculation of (Line-to-Line) or (Line) Voltages
Phasor Diagram
6/26/2014
14
27
Delta-connected Loads
Calculation of Line currents
28
6/26/2014
15
DELTA-WYE TRANSFORMATION
It simplifies calculations
• You get a neutral point
• Per-phase analysis is possible
29
(in balanced conditions)
30
PER-PHASE ANALYSIS
Why per-phase analysis ?
• If you have a balanced system
• You need to transform into Y if there is a delta-connected system
• Neutral current is zero because of balanced current (I1+I2+I3=0)
Y-connected system
• Balanced power systems are solved on a «per-phase basis».
• The other two phases carry identical currents except for the phase shift
6/26/2014
16
BALANCED THREE-PHASE POWER:
Consider a balanced three-phase circuit has the following voltages;
And consider the following set of balanced load phase-currents;
31
BALANCED THREE-PHASE POWER:
The instantaneous power of the three-phase load:
32
6/26/2014
17
After simplification;
Where
Vp: rms value of phase voltage
Ip: rms value of phase current
θ: phase angle between
voltage and current (power factor angle)
Average (real, active) power
in Watts (W), or kW, MW
Reactive power
in Vars, or kVar, MVar
Complex power
in VA, or kVA, MVA
or
or
33
34
6/26/2014
18
Solution:
35
Solution:
36
6/26/2014
19
Solution:
37
38
End of Chapter 2

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POWER SYSTEM ANALYSIS-2

  • 1. 6/26/2014 1 Chapter 2: Basic Principles (A review) 1 Power in single-phase AC circuits 2 instantaneous voltage instantaneous current instantaneous power instantaneous power is not practical to use so let’s simplify it!
  • 2. 6/26/2014 2 3 Trigonometric identity iv   Phase angle between voltage and current 4 Average value of a signal s(t) =>  T dtts T 0 )( 1 T: period Let’s first find the average value of   T VIdttpR T 0 cos)( 1  cosVIP  Average power Active power Realpower Unit is Watts (W) kW MW Since P is not zero, it is converted into other forms of energy; such as motion,heat,light,etc...
  • 3. 6/26/2014 3 5 Secondly let’s find the average value of   T dttpX T 0 0)( 1 Meaning of zero is that pX(t) does not do any work !  It is the oscillating component of instantaneous power and should be considered together with active power P  We define reactive power Q as the amplitude of this oscillating power Unit is volt-ampere-reactive (VAR) kVAR MVAR 6 BOX i(t) + v(t) For RESISTIVE component: 0 iv  No phase angle difference between voltage and current VIVIVIP  0coscos Real power associated with R 00sinsin  VIVIQ  No reactive power associated with R Proof ?
  • 4. 6/26/2014 4 7 BOX i(t) + v(t) For INDUCTIVE component:  90 iv  Phase angle difference between voltage and current 090coscos  VIVIP  No Real power associated with L VIVIVIQ  90sinsin Reactive power associated with L Proof ? 8 BOX i(t) + v(t) For CAPACITIVE component:  90 iv  Phase angle difference between voltage and current 0)90cos(cos  VIVIP  No Real power associated with C VIVIVIQ  )90sin(sin Reactive power associated with C Proof ? What is the meaning of «-» sign ?
  • 5. 6/26/2014 5 9 Let’s remember BOX theory ! BOX I + V ? + I: rms BOX current V: rms BOX voltage For the configuration above ( If i(t) enters to the BOX at (+) terminal) Consumed Produced P>0 P<0 Q>0 Q<0 In short: negative P or Q means production or generation ! Real Power Reactive Power Summary 10
  • 7. 6/26/2014 7 Complex power 13 voltage and current phasors Phasor Diagram Complex power Power triangle Apparent power Complex power balance 14 source load PG + losses QG PL QL PLoss QLoss PG=PD=PL+Ploss QG=QD=QL+Qloss SG=sqrt(PG^2+QG^2) Demand Side SD=sqrt(PD^2+QD^2) SG=SD Generation Side
  • 8. 6/26/2014 8 15 Power factor correction 16 Lagging pf Unity pf Power factor correction
  • 10. 6/26/2014 10 Complex power flow 19Bus1 Bus2 Transmission line Sflow Turkey power grid 20 Let’s find complex power flow from Bus1 to Bus2 Real power flow from Bus1 to Bus2 Reactive power flow from Bus1 to Bus2
  • 11. 6/26/2014 11 21 Which parameter(s) more or less will effect real power flow ? Realpowerflow Less effective More effective • Tight bus voltage control (around 1.0 pu) • Voltage stability concerns Real power can be effectively controlled/governed by angle difference What is the maximum possible real power flow on a line? 22 Which parameter(s) will effect reactive power flow ? Reactivepowerflow Less effective Voltage difference (more effective) • Angle difference is generally small • Transient stability concerns Reactive power can be effectively controlled/governed by voltage magnitude difference
  • 13. 6/26/2014 13 PHASE-SEQUENCE 25 Hint: check the 2nd phase (ph-B) 26 Y-connected Loads • Line-to-neutral voltages • Ref. A is chosen arbitrarily as reference • Positive sequence Calculation of (Line-to-Line) or (Line) Voltages Phasor Diagram
  • 15. 6/26/2014 15 DELTA-WYE TRANSFORMATION It simplifies calculations • You get a neutral point • Per-phase analysis is possible 29 (in balanced conditions) 30 PER-PHASE ANALYSIS Why per-phase analysis ? • If you have a balanced system • You need to transform into Y if there is a delta-connected system • Neutral current is zero because of balanced current (I1+I2+I3=0) Y-connected system • Balanced power systems are solved on a «per-phase basis». • The other two phases carry identical currents except for the phase shift
  • 16. 6/26/2014 16 BALANCED THREE-PHASE POWER: Consider a balanced three-phase circuit has the following voltages; And consider the following set of balanced load phase-currents; 31 BALANCED THREE-PHASE POWER: The instantaneous power of the three-phase load: 32
  • 17. 6/26/2014 17 After simplification; Where Vp: rms value of phase voltage Ip: rms value of phase current θ: phase angle between voltage and current (power factor angle) Average (real, active) power in Watts (W), or kW, MW Reactive power in Vars, or kVar, MVar Complex power in VA, or kVA, MVA or or 33 34