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EE742
Chap.5:ElectromechanicalDynamics
Y. Baghzouz
Fall2011
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introduction Inthischapter,alongertimescaleisconsideredduring
whichtherotorspeedwillvary(orderofseconds 10s
ofseconds transientperiod).
Thechangeinrotorspeedinteractswiththeelectro
magneticchangestoproduceelectromechanical
dynamiceffects.
Someimportantstabilityconceptswillbeintroduced
mathematicallywithphysicalimplications.
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Swingequation
Rotordynamicequation(NewtonsLawonmotion):
Atsteadystate, m= sm,and
Rotorspeed:
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SwingEquation
Aftersubstitution,
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SwingEquation
Inertiaconstant:
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DampingPower
Assumptions:
Generatorequivalentcircuitresemblesthatofaninductionmotor:
Whenignoringrotorsaliency,
where
and
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Dampingpower
Withrotorsaliency,thefollowingformulaisderivedwhenusing dqaxis
decomposition notedependencyonrotorangle.
Forsmallspeeddeviations,theaboveexpressioncanbeapproximatedby
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Dampingpower
Forlargespeeddeviationvalues,itisconvenienttorewritePDas
Criticalspeeddeviationineachaxis:
Criticaldampingpowerineachaxis:
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Equilibriumpoints
Recallthegeneratorpoweranglecharacteristicatsteadystate(chap.3):
Forsalientpole:
Forroundrotor:
Theswingequationcanberewrittenas:
Atequilibrium,
Hence, Usingpoweranglecurveforsimplicity:
NoequilibriumpointwhenPm>criticalpower
oneequilibriumpointwhenPm=criticalpower
twoequilibriumpointswhenPm
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Steadystatestabilityofunregulatedgenerator
Wefirstignorethecontrolsofthegeneratorandturbine(i.e., the
mechanicalpowerandexcitationvoltageareconstant).
Smalldisturbanceorsmallsignalstability:issystemissaidtobe
steadystatestableforaspecificoperatingconditionif,followinga
smalldisturbance,itreachesasteadystateoperatingpointator
closetothepredisturbancecondition.
Herein,thepowersystemmaybelinearizedneartheoperatingpoint
foranalytical
purposes.
Thegeneratorinfinitebusbarsystemisstableonlyinthelefthand
sideofthepoweranglecurve
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Steadystatestabilityofunregulatedgenerator
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Transientpoweranglecharacteristic
Rotoroscillationsoccurinthesametimescaleasthetransient
period generatormodelduringtransientstate: Forgeneratormodelwithconstantfluxlinkage,seeFig.below(Chap.4)
Round
rotorSalient-pole
rotor
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Transientpoweranglecharacteristic
Constantfluxlinkagemodel:
Forageneratorwithasalientpolerotor,
theabovetransientpowerexpressionsimplifiesto
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Transientpoweranglecharacteristic
Classical
generator
model: theconstantfluxlinkagemodelcanbesimplifiedfurtherbyignoringthetransientsaliency,i.e.,assuming
that Thetransientpowerequationbecomesequalto
Notethat
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Examples5.1
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Examples5.2
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Impactofincreaseinload
Theincreaseinload modifiesthetransientcharacteristicasshownbelow(resultsinsmallertransientemfE,hencesmallerpeakvalue
ofthetransientpowercurve).
Thetransientsynchronizingpowercoefficient
issteeperthanitssteadystatecounterpart
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Effectofdamperwinding
Forsmalldeviationsinspeed,thedamperwindingproducesdampingpowerthatisproportionaltospeeddeviationandaddsuptothe airgap
power.ThesignofPDdependsonthesignof .
Therotorwillthereforemovealongamodifiedpowerangletrajectory.
Startingfrompoint2,therotor
beginsto
decelerate
and
reaches
minimumspeedatpoint6.
Pastpoint6,therotoraccelerates
andreachessychronous speed
whenarea246=area635
Therotoroscillationsaredamped
andthesystemquicklyreaches
theequilibriumpoint1.
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Effectofrotorfluxlinkagevariation
Inreality,E isnotconstant (asthearmaturefluxenterstherotorwinding,therotorfluxlinkagechangeswithtime).
Tosimplifytheanalysis,onlythesalientpolemachineisconsidered
(i.e., ))
Linearizethetransientpowerequationattheinitialoperatingpoint:
where Eq canbe inphasewiththespeeddeviation inthiscase,it
inducesanadditionaldampingtorque,(seefirstfigurebelow).
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Effectofrotorfluxlinkagevariation
Updatednecessaryconditionforsteadystatestability(i.e., Eq tobeinphasewiththespeeddeviation ):
Incaseoflargenetworkresistance, Eq canbe180o outofphasewith
thespeeddeviation, generatorinstability canoccurifthisnegative
dampingislargerthatthepositivedampingproducedbythedamper
winding(seesecondfigurebelow).
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Rotorswingsaroundtheequilibriumpoint
Linearizedswingequation:
Rootsofcharacteristicequation:
Threepossiblesolutions:underdamped,criticallydampedandover
damped.
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Mechanicalanaloguesofgeneratorinfinitebus
barsystem Dynamicequationofmassspringdampersystem
Dynamicequationofpendulum(notincludingdamping)
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Steadystatestabilityofregulatedsystem
(whenaction
of
AVR
is
included)
Studyrestrictedtogeneratorwithroundrotorandnegligible
resistance.
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SolveforEqintermsofVs,Vg,and :
Substituteinthepowerequation:
The AVR increases the amplitude
of the power curve significantly
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GeneratorpowerisproportionaltoEqb.
Maximumpoweroccurswhen
Dashed curves 1-6 represent
PEq
() for higher values of Eq.
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TheslowactingAVR(onewithalargetimeconstant)willnotbeable
torespondduringthetransientperiod,hencethestabilitylimitcorrespondsto = /2.
For afastactingAVR(withshorttimeconstant),thestabilitylimit
correspondsto > /2.ThisvaluedependsonthesystemandAVR
parameters(i.e.,conditional
stability).
Theinfluenceoffieldcurrentlimiter isillustratedinthefigurebelow.
Thefieldcurrentlimitisreachedbefore PVgMAX ifXissmall.
Belowthelimitingpoint,thegeneratorsteadystatecharacteristicfollowsPVg.
Abovethelimitingpoint,thegeneratorsteadystatecharacteristicfollowsPEq.
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Transientpoweranglecharacteristicsofregulated
generator
WeconsiderAVRwithlargetimeconstant.Inhere,thetransient
characteristicsisthesameastheunregulatedsystemexcept,
thevalueofEq ishigher(hencehigheramplitudeofPE())sincetheincreased
loadingin
the
regulated
system
causes
an
increase
in
the
steady
state
field
current.
Inaddition,theangle reaches/2beforereacheditscriticalvalue.
Notethat whenthe reacheditscriticalvalue, > /2,henceKE is
negative.SoatwhichpointonthePVg()curvewhenKE=0?
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UsingclassicalmodelandphasordiagraminFig.20b,
RatioofpoweratwhichKE=0tothepoweratwhichKVg=0:
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isstronglydependentonthesystemreactanceX.
Refertothefiguresbelow:
AtoperatingpointA(lightload),0
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Effectorrotorfluxvariation
Determinethephaseshiftbetweenspeedchangeand (seeSection5.5.3fordetails)
ThephasorsbelowshowrepresenttwotypesofAVRs:
ForstaticexciterEfisinphasewithV
Forrotatingmachineexciter,EflagsVby10s ofdegrees. theoutofphasecomponent relativeto reducesdamping(i.e.,
increaseschancesofinstability).
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