Hamilton Power Systems

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    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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