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8/8/2019 Hamilton Power Systems
1/25
Copyright 2005 W.O. (Bill) Kennedy
Power Systems
for the
Non-Power Engineer
Hamilton Section
February 25, 2005
W.O. (Bill) Kennedy, P.Eng., FEIC
IEEE Canada President
Copyright 2005 W.O. (Bill) Kennedy
1 23
56
7
8
50 MW
25 MVR
80 MW
40 MVR
205 MW
103 MVR
9 10 11
95.00 MW
1 MW
1 MVR
51.50 MW51.50 MW51.50 MW
6 .0 0 M VR 6 .0 0 M VR 1 1. 00 MV R
5.10 MVR
0.00 MVR
95.00 MW
1.02 pu
-4.62 Deg
0.99 pu
-11.01 Deg
1.06 pu-2.43 Deg
88.4 MVR
Copyright 2005 W.O. (Bill) Kennedy
Purpose
Give you a basic understanding of what
power systems are and how the
components fit together and work
Concepts will be emphasized
Mathematics will be kept to a minimum
Mathematics only when necessary
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Copyright 2005 W.O. (Bill) Kennedy
Introduction
First part covers power system
components
Second part covers how the
components fit together and work
along with some measures of
power system performance
Copyright 2005 W.O. (Bill) Kennedy
A little bit of Physics
Hans Christian Oerstead discovered therelationship between magnetism andelectricity
Michael Faraday discovered that avoltage is induced on a wire when it wasmoved in or through a magnetic field
James Clerk Maxwell developed themathematics of electromagnetics
Copyright 2005 W.O. (Bill) Kennedy
Real and Reactive Power
Real power does the work
Reactive power helps real power
do the workPower systems need both or they
wont work
What is reactive power?
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Copyright 2005 W.O. (Bill) Kennedy
Reactive power
Quarterback can
throw a bullet, butnot very far
For long distances,throws in an arc
Real power is thebullet
Reactive power isthe height of the arc
Copyright 2005 W.O. (Bill) Kennedy
Reactive Power Capacitors store energy equal
to CV2
Capacitor banks are used to
boost or raise voltage
Reactors use energy equal to
LI2
Motors and fluorescent lights
require reactive power
Copyright 2005 W.O. (Bill) Kennedy
Part 1 - Equipment
Generators
Transformers
Transmission Lines
Loads
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Copyright 2005 W.O. (Bill) Kennedy
Generators
Copyright 2005 W.O. (Bill) Kennedy
Generators
Fundamental Law
E = N d/dt
Where is the flux
Magnetic example
High school physics
Faraday's discovery motion
Maxwell mathematical theory
Copyright 2005 W.O. (Bill) Kennedy
Generators
Rotor turns inside of the generator
satisfying Faradays Law
Voltage induced on the stator followsa sine wave
Take advantage of space and put three
coils equally spaced, 120o apart
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Copyright 2005 W.O. (Bill) Kennedy
GeneratorsThree Phase
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
0 45 90 135 180 225 270 315 360
Degrees
Magnitude
Phase A
Phase B
Phase C
Motion of rotor induces a voltage on the stator
Stator doesnt move and waveform reflects effect of
rotor field as it moves inside the machine
Copyright 2005 W.O. (Bill) Kennedy
Generators
ControlTerminal voltage
Speed
Terminal voltage controlled by varyingthe voltage applied to the dc field of therotor
Speed controlled by governor, as loadincreases, fuel supply increases
Copyright 2005 W.O. (Bill) Kennedy
Generators
Speed and frequency (60 Hz)
Frequency (f) = n/60 * p/2
Poles are in pairs, hence divide by 2
Speed in revolutions per minute, whereas
frequency in cycles per second, hence
divide by 60
Steam sets high speed, small rotors
Hydro sets low speed, big rotors
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Copyright 2005 W.O. (Bill) Kennedy
Generators
Two pole machine
rotates at 3600 rpm steam generator
Twelve pole
machine rotates at
600 rpm hydro set
Copyright 2005 W.O. (Bill) Kennedy
GeneratorsGeneration by Fuel Type (Canada)
14%
53%
3%
10%2%
16%
2%
0%
coal
nuclear
hydro
oil
gas
dual fuel
pumped storage
other
Prime mover drives the generator
Energy sources in Canada
Copyright 2005 W.O. (Bill) Kennedy
Generators
Capability curve
Limits
Stator heating
Rotor heating
Stability
Whats required
Whats used
Generator CapabilityCurve
-1
-0.8
-0.6
-0.4
-0.2
0
0.20.4
0.6
0.8
1
0.00 0.25 0.50 0.75 1.00
Real PowerReactivePower
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Copyright 2005 W.O. (Bill) Kennedy
Generator Capability Curve
-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
0.00 0.25 0.50 0.75 1.00
Real PowerReactivePower
Copyright 2005 W.O. (Bill) Kennedy
Transformers
Follow Faradays Law
E1=N1d/dt & E2=N2d/dt
Flux (d/dt) is constant
Voltage change depends on number of
turns, and basic equations can be
equated with the result:
E1/N1 = E2/N2
Copyright 2005 W.O. (Bill) Kennedy
Transformers
Since conservation
of energy must be
preserved and
voltage variesinversely, current
must vary directly
I1N1 = I2N2
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Copyright 2005 W.O. (Bill) Kennedy
Transformers
Usual connection for the transmission systemis WYE grounded at the high voltage
Generators connected DELTA
Loads can be both
Copyright 2005 W.O. (Bill) Kennedy
Transmission lines
Transmission lines are the highways onwhich power travels
Losses are proportional to the currentsquared on the line times the resistance
Want highest practical voltage tominimize losses
As we will see, SIL is an importantproperty of transmission lines
Copyright 2005 W.O. (Bill) Kennedy
Surge Impedance Loading
(SIL)
Transmission line
consists of:
Shunt capacitance
Series resistance and
inductance
Distributed along length
of line
Treat as distributed
lumped elements
Can ignore resistance
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Copyright 2005 W.O. (Bill) Kennedy
Surge Impedance Loading
(SIL)
Close the breaker at
sending end Shunt capacitance
charges to CV2
Close the breaker at
receiving end and feed
the load
Series inductance uses
energy at LI2
Load
Load
Copyright 2005 W.O. (Bill) Kennedy
Surge Impedance Loading
(SIL)
Equating shunt and series energies
CV2 = LI2
Performing the math yields
SIL (power) = V2/SI
Copyright 2005 W.O. (Bill) Kennedy
Properties of Surge Impedance (SI)
Remains fairly constant over a wide range ofvoltages
Starts around 400 at lower voltages and
decreases with bundling to around 225 at1500 kV
Capacitance and inductance also remainconstant
Using this we can construct the followingtable
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Copyright 2005 W.O. (Bill) Kennedy
Properties of Transmission Lines
Voltage (kV) SI () R ( /km) X ( /km) Charging(kVAr/km)
SIL(MW)
X/R
69/72 370 0.4 0.5 15 13/14 1.2
138/144 370 0.2 0.5 70 50/55 2.5
230/240single
340 0.07 0.45 225 170 6
230/240bundled
300 0.07 0.4 290 180/195 6
345 bundled 285 0.026 0.365 525 415 14
500 bundled 250 0.018 0.345 1340 990 20
Copyright 2005 W.O. (Bill) Kennedy
St. Clair Curve
0.00
0.25
0.50
0.75
1.00
1.25
1.50
1.75
2.00
2.25
2.50
2.75
3.00
3.25
100
200
300
400
500
600
700
800
900
1000
Length (km)
LineLoading
(SIL)
Copyright 2005 W.O. (Bill) Kennedy
Loads
Three types of load models
Constant MVA motors
Constant current resistive loads Constant impedance reactor & capacitor
banks
For power flow use constant MVA
For transient studies need a combination and
may require frequency
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Copyright 2005 W.O. (Bill) Kennedy
Summary Part 1
Generators make the product
Transformers raise and lower voltageto allow efficient transport of product
Transmission lines are the highways
Loads are the end user of the product
Copyright 2005 W.O. (Bill) Kennedy
Time for a BreakTime for a Break
Copyright 2005 W.O. (Bill) Kennedy
Characteristics of power systems
Generation is usually remote from loads
Transmission needed to connect generationto load
Transformers needed to raise/lower voltage Want as high a voltage as practical fortransmission minimizes losses
Use load size, generator size and line SIL toget line voltage
In Saskatchewan, lines are typically 170 kmlong
At that distance loading 2 times SIL
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Copyright 2005 W.O. (Bill) Kennedy
Putting it all together
Generators produce real power (P)
Generators produce/consume
reactive power (Q)
Generator Q for underexcited
operation is around half overexcited
ability
Copyright 2005 W.O. (Bill) Kennedy
Putting it all together
Transmission lines consume P in formof losses, typically 5% to 7% ofgeneration
Lines produce/consume Q dependingon power flow on the line as a fractionof SIL< SIL VArs flow out of line
> SIL VArs flow into line
Half from each end, if voltages are equal
Copyright 2005 W.O. (Bill) Kennedy
Putting it all together
Loads consume P & Q
P required for resistive loads
Q required for reactive loads induction motors
Synchronous motors can produce/consume Q
Switching and/or load stations
Use shunt reactor/capacitor banks to
produce/absorb Q
Primarily for voltage control
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Copyright 2005 W.O. (Bill) Kennedy
Breakers
Breakers used toconnect/disconnect
equipment
Breakers must be
capable of picking
up and dropping
loads
Copyright 2005 W.O. (Bill) Kennedy
Breakers
Breakers must becapable of switchingunloadedtransmission lines
Breakers must becapable ofinterrupting thesymmetrical faultplus any dc offset
Copyright 2005 W.O. (Bill) Kennedy
How the power system works
Fundamental rules
Maintain reactive power balance and
voltages will be in required range typically +/- 5% of nominal
Maintain load/generation balance and
frequency or speed remains constant
typically 60 Hz +/- 0.02 Hz
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Copyright 2005 W.O. (Bill) Kennedy
Power flow
To solve a power flow need to solve for four
variables at each bus Bus voltage V
Bus angle
Real power P
Reactive power Q
However, some variables already known
Load P & Q
Generator bus V
Copyright 2005 W.O. (Bill) Kennedy
Power flow
Need a model of the system
Per unit system is best
Must have consistent voltage ratios
Base impedances on voltage level
Most models involve some lumping, i.e.not practical to model every detail
However, this depends on the type ofstudy
Copyright 2005 W.O. (Bill) Kennedy
Solution methods
Four solution methods
Gauss-Siedel solves vector equations
Newton-Raphson solve for P & Q by
separation of variables
dc solves circuit as a dc circuit by
treating jX as a resistance
Decoupled load flow variant of Newton-
Raphson. Separates V &
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Copyright 2005 W.O. (Bill) Kennedy
Solution methods
Solution results
Balance generation with load and lossesKeep all bus voltages within tolerance +/-
5%
Require a slack or swing bus. Can be afictitious generator to supply/absorb P & Q
Solution achieved when swing bus P & Qequal zero
Not practical, therefore minimize swing busP & Q
Copyright 2005 W.O. (Bill) Kennedy
Types of studies
Steady state studies
Operations study effect today and
tomorrow, usually short time, e.g. up to
one month
Planning study effect of load and
generation three or more years in future
Fault study what happened yesterday
Copyright 2005 W.O. (Bill) Kennedy
Types of studies
Dynamic studies
All of the above: Operations, Planning &Fault
Transients what happens as powersystem moves from one steady state toanother
Additional studies determine equipmentratings, e.g. breaker duty
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Copyright 2005 W.O. (Bill) Kennedy
Contingencies
Contingencies test the system for
robustnessContingency loss of one or more
components at a time
Costs escalate if system designed formore than two contingencies
Example loss of a generator and line ortransformer N-G-1 (NERC category C)
Copyright 2005 W.O. (Bill) Kennedy
Power system example
1 23
56
7
8
50 MW
25 MVR
80 MW
40 MVR
205 MW
103 MVR
9 10 11
95.00 MW
1 MW
1 MVR
51.50 MW51.50 MW51.50 MW
6 .0 0 M VR 6 .0 0 M VR 1 1 .0 0 M VR
5.10 MVR
0.00 MVR
95.00 MW
1.02 pu
-4.62 Deg
0.99 pu
-11.01 Deg
1.06 pu-2.43 Deg
88.4 MVR
Copyright 2005 W.O. (Bill) Kennedy
Power System Performance
WAMS Wide Area MeasurementSystems
Losses weve ignored losses upto this point
Measuring outages
Lines & Stations
Delivery Point measures
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Copyright 2005 W.O. (Bill) Kennedy
WAMS
Slow speed synchronized
measurements of voltages, power andfrequencies on a power system
IEEE Standards PC37.118 in votingstage
Want to capture slow-speed events
High-speed events captured by faultrecorders
Copyright 2005 W.O. (Bill) Kennedy
Synchrophasor Standard
PC37.118 Standard defines measurement, accuracy & test
requirements (includes timing requirements)
Phasor
Measurement
Unit (PMU)
UTC Time
(GPS)
X(n) = Xr(n) +jXi(n)X = Xr +jXi
X
Xi
X r
X(n)
Xi(n)
X r(n)
Phasor defined
at t = 0.
Waveform matchesphasor definitionat t = 0.
PMU estimates phasorequivalent from an intervalof the waveform.
The estimate is comparedwith the defined phasor todetermine error (TVE).
= [((Xr(n) - X
r) 2 + (X
i(n) - X
i) 2 ) / (X
r
2 + Xi
2 )]-1
-0.5
0
0.5
1
- 0. 01 2 - 0. 00 8 - 0. 00 4 0 0 .0 04 0 .0 08 0 .0 12
Copyright 2005 W.O. (Bill) Kennedy
Phasor Systems in WECC PMU to PDC, real time
BPA - 15 in NW, 1 in CAL
SCE - 14 in S. CAL &NEV
PG&E - 6 in N. CAL
PNM - 2 in NM
WAPA - 3 in COLO & NM
BC Hydro - 6 in BC
APS/SRP - 5 in AZ & NM
PMU to stored files Alberta ISO - 4 in Alberta
2nd Level, PDC-PDC SCE -BPA
WAPA - BPA
BPA & SCE to Cal ISO
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Copyright 2005 W.O. (Bill) Kennedy
S u m m a r y P lo t F o r 0 2 1 0 0 8 N W G e n D r o p _ A l l A n g s
0 2 1 0 0 8 N W G e n D ro p _ A llA n g s 1 2 / 1 3 /0 2 _ 1 2 :5 9 :1 2
S Y L M S y l m a r B u s V o l t a g e V A n g R M F 0 1
A U L T 3 4 5 k V B u s V o l t a g e ( C r a i g ) V A n g R M F 0 2
B E A R 3 4 5 k V B u s V o l t a g e ( C r a i g ) V A n g R M F 0 2
S H I P 3 4 5 k V B u s V o l t a g e ( S a n J u a n ) V An g R M F 0 2
I N G 1 5 L 5 2 C u s t e r V o l t a g e V A n g R M F 0 3
D M R 1 5 L 2 9 M a l a s p i n a V o l t a g e V A n g R M F 0 3
N I C 1 5 L 8 1 I n g l e d o w V o l t a g e V A n g R M F 0 3
A B 0 1 C a l g a r y V A n g R M F 0 4
P i n n a c l e P k B u s V A n g R M F 0 5
0 5 1 0 1 5 2 0 2 5 3 0 3 5 4 0 4 5- 2 0 0
- 1 0 0
0
10 0
20 0
30 0
40 0
T i m e i n S e c o n d s s i n c e 0 8 - O c t - 2 0 0 2 2 2 : 3 1 : 1 5 . 5 3 1
S y l m a r
BC H
C a l g a r y
P i n n a c l e P k
S h i p r o c k
A u l t / B e a r s E a r s
D M W G / j f h
Copyright 2005 W.O. (Bill) Kennedy
Chief Joseph dynamic brake 1400 MW
toaster
Three 230 kVstructures
Resistive wirestrungthroughpulleys
Limited timeduration .5 sec
normal
2 sec limit
Cool-offrequired
Copyright 2005 W.O. (Bill) Kennedy
Dynamic brake detail
Lower
brackets with
pulleys and
weights for
tension
Pulley section
adjusts for
ambient and
loading
temperature
changes
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Copyright 2005 W.O. (Bill) Kennedy
RAS initiated
Dynamic
Brake
Faulted PT causesbus outage
RAS triggers Brake Low Volt
Power flow drop
No gen drop initiated
Long fault causesmore significantringdown networkresponse
No net systemeffects
Copyright 2005 W.O. (Bill) Kennedy
Transmission Losses
Transmission Losses
0
100
200
300
400
500
4 75 0 5 00 0 5 25 0 5 50 0 5 75 0 6 00 0 6 25 0 6 50 0 6 75 0 7 00 0 7 25 0 7 50 0 7 75 0
NetGeneration toSupply Alberta Load(MW)
Losses
(M
W
)
Losses are
stochastic
Simple system
losses vary as a
square of current
Complex system
losses display a
linear variance
Copyright 2005 W.O. (Bill) Kennedy
Transmission LossesTransmission Losses Histogram
0
100
200
300
400
500
197
210
223
236
249
262
275
288
301
314
327
340
353
366
379
392
405
418
431
Losses (MW)
Coun
t
Histogram demonstrates a normal
distribution pattern for losses
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Copyright 2005 W.O. (Bill) Kennedy
Transmission lossesTransmission Generation, Load and Losses by Day
4000
4500
5000
5500
6000
6500
7000
7500
1 2 3 4 5 6 7 8 9 1 0 11 12 13 14 15 16 17 18 1 9 20 21 22 2 3 24
Hour
Geenration&Load(MW)
0
100
200
300
400
500
600
700
800
900
1000
Losses(MW)
Net Gen
Net Load
Losses
+3-sigma-3-sigma
Ave Losses
Losses on AIES are very l inear
Copyright 2005 W.O. (Bill) Kennedy
Power system performance
Need measure system performance
Measure frequency and duration ofoutages
Reason outages occur infrequently
Measures of performance look at allcomponents and causes
Usually stated as an average of wholesystem
Copyright 2005 W.O. (Bill) Kennedy
Performance
For Alberta, AESO publishes data to itswebsite on line and terminal outages asan overall average for the voltage class
For Delivery Points frequency andduration data also published as asystem average
For comparison, all Canada data isincluded for Delivery Points
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Copyright 2005 W.O. (Bill) Kennedy
Performance
Two types of duration are measured
Momentary < 1 minute
Sustained > 1 minute
Following are examples of charts
published on the AESO website
http://www.aeso.ca/transmission/5548.html
Copyright 2005 W.O. (Bill) Kennedy
Transmission - line
1.721,7010.05%6.074,5980.7675798,997Total
5.96950.03%2.64370.88141,595500
0.943200.04%4.931,1590.6923533,968240
1.266850.05%7.062,2720.5932254,417138/144
6.676010.14%6.081,1302.061869,01769/72
Frequency
per 100 km.a(faults/100
km.a)
Number ofMomentary
Faults
Unavailabilityper 100 km.a
(%)
Average
OutageDuration(hrs/fault)
Total
OutageDuration(hours)
Frequency
per 100 km.a(faults100
km.a)
Number ofSustained
Faults
KilometerYears(km.a)
VoltageClass (kV)
For the Period From 1997 - 2001
Summary for Line Related Forced Outages
Transmission Outage Statistics
Alberta Interconnected Electric System
Copyright 2005 W.O. (Bill) Kennedy
System Average Interruption Frequency
SAIFI-MI
0.0
0.4
0.8
1.2
1.6
1 997 1 99 8 1 99 9 2 00 0 2 00 1
Year
Frequency
Alberta
Canada
Ice StormRemoved
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Copyright 2005 W.O. (Bill) Kennedy
System Average Interruption Duration
SAIDI
0
100
200
300
400
1 997 1 998 19 99 20 00 20 01
Year
Duration(minutes) Alberta
Canada
Ice StormRemoved
Copyright 2005 W.O. (Bill) Kennedy
Summary
Generators make the product
Transformers raise and lower thevoltage and current to allow efficienttransport of the product
Transmission lines are the highwaysthat allow the power to flow from thegenerator to the load
Loads are the end user of the product
Copyright 2005 W.O. (Bill) Kennedy
Summary Part 2
Power flow studies model and test
the system for robustness
yesterday, today and tomorrowN-G-1 (NERC C) is used to test
the system for operation today and
into the future
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Copyright 2005 W.O. (Bill) Kennedy
Summary Part 2
Losses are an important part of
power system design and operation
Higher voltage lines reduce losses
However, losses are fixed when the
conductor is chosen
Must do a conductor optimization
study
Copyright 2005 W.O. (Bill) Kennedy
Summary Part 2
Outages are measured using
frequency and duration techniques
Presented as system average
numbers
Copyright 2005 W.O. (Bill) Kennedy
Summary
Power systems are mankinds most complex
machine
Power systems cover thousands of square
kilometers Supply thousands of customers all day -
everyday
Must always work together generally do
Must supply power and energy when
requested ultimate Just in Timesystem
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Copyright 2005 W.O. (Bill) Kennedy
Thats all folks!
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