Upload
hadan
View
248
Download
0
Embed Size (px)
Citation preview
H I G H - P O W E R E D R E S E A R C
H F
OR
TH
E R
EA
L W
OR
LD
December2011Issue…
1 ModelingCurrentTransformer(CT) SaturationforDetailedProtectionStudies
6 TheWoundRotor(WR)andSquirrel Cage(SQ)InductionMachineModels inthePSCAD®Library
9 NewPTConnections
11 MeettheTeam!
12 PSCAD®2012TrainingSessionsDecember 2011
ThePSCAD®MasterLibrarycontainsanumberofmodelsthatcouldbeusedfordetailedprotectionsystemanalysis. Themostimportantofthesemodelsarethecurrenttransformermodels.Currenttransformersaturationisassociatedwithmanyprotectionproblemsencounteredinpowersystems.CTsaturationisacomplexphenomenonandaccuratemodelinginasimulationenvironmentischallenging.ThemodelsavailableinPSCAD®arebasedontheadvancedmathematicalmodelsproposedbyJilesandAthertonandcommonlyreferredtoasthe
‘Jiles-AthertontheoryofFerromagnetichysteresis.’
ThesedevelopedmodelshavebeenextensivelytestedwithfieldrecordingsincollaborationswithCT,relayandprotectionequipmentvendors.
ThiscaseisusedtoillustratetheeffectsofCTsaturation.ThekeyparametersthatimpactCTsaturationarediscussedinanefforttoguidePSCAD®userswhomayusethismodelfortheirsimulations.
GeneralTheory ThemagneticcharacteristicoftheCTisshowninFigure1(hysteresisnotshown).Inthelinearregion,theCTwillbehavealmostlikeanidealratiochanger.Thatis,theCTsecondarycurrentisanidenticalbutscaleddownreplicaoftheprimarycurrent.However,IftheCTsaturates,morecurrentisrequiredtomagnetizethecoreandasaresultthesecondarycurrent(IS)availableasinputstotherelay
maynotbeanidenticalscaleddownreplicaoftheactualprimarycurrent(IP).Thiscanleadtoprotectionissuesandshouldbegivendueconsideration.
SystemOverview TheACsystemshowninFigure2consistsoftwo230kV,60HzThevaninvoltagesources,a75MVAloadandthree230kVtransmissionlines(125km,75kmand200km).Asinglephase(PhaseA)togroundfaultisappliedbetweenthefirsttwotransmissionlines.
ModelingCurrentTransformer(CT)SaturationforDetailedProtectionStudiesDr. Dharshana Muthumuni, Lisa Ruchkall, and Dr. Rohitha Jayasinghe, Manitoba HVDC Research Centre
Figure1 IM–Fluxcurve
2 P U L S E T H E M A N I T O B A H V D C R E S E A R C H C E N T R E J O U R N A L
CurrentTransformerSaturation CTsaturationcanbeexplainedusingthesimplifiedequivalentcircuitshowninFigure3.
Inthelinearregionofoperation,magnetizingcurrent(IM1)isverysmallandhenceIP–IMisapproximatelyequaltoIP.ThusISwouldbeascaleddownversion(byafactorofN).IftheCTsaturates,themagnetizingcurrentincreases(IM2).Asaresult,onlyapartofIPisavailablefortransformationtothesecondary.Inthissimulationcase,afaultissimulatedonthetransmissionlineandtheCTisattheendoftheline(whereIabcismeasured).
Note:Figure4showshowtheCTmodelisusedinPSCAD®.Notealsothattheinputprimarycurrent(Iabc)isinkiloampsandthesecondarycurrent(Isabc)isinamps.TheCTsaremodeledas(independent)blocksanddonothavetobeconnectedtotheelectriccircuit.
ThisrepresentationisvalidsincetheCTisessentiallyashortcircuit(inseries)fromtheprimarypowersystemnetworkperspective.
KeyParametersImpactingCTSaturationThefollowingcanhaveasignificantimpactonCTsaturationandshouldbegivendueconsiderationinasimulationstudy:
1) DCoffsetintheprimarysidefaultcurrent.2)RemnantfluxontheCTpriortothefault(ifany).3)Secondarysideimpedanceincludingthoseof therelay,connectingwiresandCTsecondary impedance-thisparameterplaysamajorrolein thelevelofsaturationtheCTwillbesubjectedto.
Illustrativesimulationresultsarepresentedinthefollowingsectionstohighlightsomeofthekeypoints.
Figure2 ACsystemmodel
Figure3 SchematicrepresentationofCT(left)andthesimplifiedequivalentcircuit(right)
Figure4 CTPSCAD®implementation
D E C E M B E R 2 0 1 1 3
Case1–Impact of DC offset in the primary fault current:ThepointonthevoltagewaveformattheinstantofthefaultdeterminestheleveloftheDCoffsetintheprimarycurrent.ThemaximumDCoffsetwilloccurwhenthefaultisappliedatavoltageminimum(t=0.49167s).TheresultsinFigure5aoccurwhentheDCoffsetissignificant.
Ascanbeseen,theDCoffsetcausestheflux(Figure5b)tobedrivendownandintosaturation.TheCThassaturatedafterabouttwocycles.ThereductionofthesecondarycurrentisevidentfromFigure5a.
ThesimulationresultsinFigure5bdemonstrateasituationwhenthereisnoDCoffset(faultisappliedatt=0.4876s,voltagemaximum).Ascanbeseen,theCTdoesnotgointosaturationandonlyasmallamountofmagnetizingcurrentisrequiredtomagnetizethecore.Therefore,thesecondarycurrentisanexactbutscaleddownreplicaoftheprimarycurrent.
InFigure5aalsonotetheremnantfluxintheCTcoreoncethefaultiscleared.EffectsofremnantfluxwillbediscussedinCase2.
Figure5a DCoffsetpresent Figure5b NoDCoffsetpresent
Main : Graphs
0.450 0.500 0.550 0.600 0.650 0.700 0.750 0.800 0.850
-200
-100
0
100
200
Volta
ge (k
V)
Vabc
-30
-20
-10
0
10
20
Sec.
Cur
rent
(A)
Ia_sec
-6.0
-4.0
-2.0
0.0
2.0
4.0
Pri.
Cur
rent
(kA)
Iabc
-1.00
-0.50
0.00
0.50
1.00
1.50
Flux
den
sity
(T)
B
Main : Graphs
0.450 0.500 0.550 0.600 0.650 0.700 0.750 0.800 0.850
-200 -150 -100 -50
050
100150200
Volta
ge (k
V)
Vabc
-30
-20
-10
0
10
20
Sec.
Cur
rent
(A)
Ia_sec
-6.0
-4.0
-2.0
0.0
2.0
4.0
Pri.
Cur
rent
(kA)
Iabc
-2.00
-1.50
-1.00
-0.50
0.00
0.50
Flux
den
sity
(T)
B
Main : Graphs
0.450 0.500 0.550 0.600 0.650 0.700 0.750 0.800 0.850
-200
-100
0
100
200
Volta
ge (k
V)
Vabc
-30
-20
-10
0
10
20
Sec.
Cur
rent
(A)
Ia_sec
-6.0
-4.0
-2.0
0.0
2.0
4.0
Pri.
Cur
rent
(kA)
Iabc
-1.00
-0.50
0.00
0.50
1.00
1.50
Flux
den
sity
(T)
B
Main : Graphs
0.450 0.500 0.550 0.600 0.650 0.700 0.750 0.800 0.850
-200 -150 -100 -50
050
100150200
Volta
ge (k
V)
Vabc
-30
-20
-10
0
10
20
Sec.
Cur
rent
(A)
Ia_sec
-6.0
-4.0
-2.0
0.0
2.0
4.0
Pri.
Cur
rent
(kA)
Iabc
-2.00
-1.50
-1.00
-0.50
0.00
0.50 Fl
ux d
ensi
ty (T
)B
Impact of DC offset in the primary fault current...
4 P U L S E T H E M A N I T O B A H V D C R E S E A R C H C E N T R E J O U R N A L
Note:theB-HlooptrajectoryoftheCTduringthefaultisshowninFigure6.TheformationoftheminorB-HloopsandhysteresisareaccuratelymodeledbasedontheJiles-Athertontheoryofferromagnetichysteresis.SuchdetailedrepresentationsoftheCTbehaviorarenecessaryfordetailedprotectionsystemanalysis,suchas:
•CTresponseduringautoreclose•ProtectionschemeswithCTsoperatinginparallel –6CTsinparallelinathree-phasetransformer differentialscheme –3CTsinparallelinanearthfaultrelayscheme – CTconnectionsingeneratorprotections
Case2–Reclosing the line while the fault is still present (auto reclose):Inthefirstfaultevent,saturationhadtakenapproximatelytwocycles.Ifthelineisreclosedwhilethefaultisstillpresent,theCTmaysaturatemuchfasterduetothepresenceoftheremnantflux.ThisisdemonstratedinFigure7.Ascanbeseen,thesaturationoccursinapproximatelyhalfacycle,possiblybeforetherelayhadtimetorespond.
Figure7 Case2results
Figure6 B-Hlooptrajectory
D E C E M B E R 2 0 1 1 5
Figure8 Case3results
Case3–Effect of the secondary impedance:TheCTsecondarysideburdenimpedancehasasignificantimpactonCTsaturation.InCase1,theburdenwassetto2.5Ω.TheresultsshowninFigure8wereobtainedbyreducingtheburdento0.5Ωinthesimulation.Ascanbeseenfromtheresults,thefluxisnotdrivendownasfar.ItalsotakesalongertimefortheCTtobecomesaturated(approximately6cycles).
Note:TheCTmodelusedintheexamplecaseisthatofasingleCToperatingindependentlyofanyotherCTsintheprotectionscheme.Ingeneral,aprotectionschememayhaveanumberofCTsoperatinginparallel.TheresponseofoneCTmayimpactthebehaviouroftheotherandthus,shouldbeappropriatelymodeled.ContactthePSCAD®TechnicalSupportTeamformoreinformationonspecificmodels.
Main : Graphs
0.450 0.500 0.550 0.600 0.650 0.700 0.750 0.800 0.850
-30.0 -25.0 -20.0 -15.0 -10.0 -5.0 0.0 5.0
10.0 15.0
A
Ia_sec
-5.0
-4.0
-3.0
-2.0
-1.0
0.0
1.0
2.0
3.0
kA
Iabc
-2.00
-1.50
-1.00
-0.50
0.00
Flu
x de
n
B
The response of one CT may impact the behaviour of the other and should be appropriately modeled…
6 P U L S E T H E M A N I T O B A H V D C R E S E A R C H C E N T R E J O U R N A L6 P U L S E T H E M A N I T O B A H V D C R E S E A R C H C E N T R E J O U R N A L
Dr. Dharshana Muthumuni, Manitoba HVDC Research Centre
TheinductionmachinemodelsaretwoofthemostwidelyusedcomponentsfromthePSCAD®MasterLibrary. ThePSCAD®libraryhastwoinductionmotormodels:
1)Squirrelcageinductionmachinemodel representingadoublecagedesign–(SQ).2)Woundrotorinductionmachinemodel–(WR).
TheTechnicalSupportTeamreceivesquestionsfromourusersastowhichmodeltheyshouldusetorepresentasetofspecificdataprovidedbytheequipmentvendor.ThegoalofthistechnicalnoteistoprovidethenecessaryinformationtohelpPSCAD®userswhenfacedwithsuchquestions.
Mathematically,theSQcagemachinecanberepresentedbytheWRmachine.TheWRmodelcouldalsobeusedtorepresentadoublecageSQmachine.Thetwoexamplesbelowwilldescriberelevantdataentryconsiderationsandalsocompareresultsforvalidationpurposes.
Thesimplesimulationcaseshownbelowisusedtohighlightthekeypoints.ASQmachineandaWRmachinewithcomparableparameters(identicalratingsanddata)areconnectedtothesamesupplysource(60Hz,0.69kV).
Example1:Modelingasinglecageinductionmachine TheSQcagemachinemodelortheWRmachinemodelmaybeusedtorepresentasinglecage(SQ)machine(IM_study_01.pscx).
Theequivalentcircuitofadoublecagedesign(asimplementedinPSCAD®)squirrelcagemachineisshownbelowinFigure2.
Theequivalentcircuitofawoundrotormachinemodel(singlerotorwinding)isshowninFigure3.
TousetheSQcagemachinemodeltorepresentasinglecagemachine:
–Makethe‘secondcageresistance’(RC2)and the‘secondcageunsaturatedreactance’(XLC2) relativelylarge(comparedtotheotherleakage inductances/resistances).Inthiscase,thevalues usedareRC2 =5PUandXLC2 =5PU,whichismuch largerthanRC1 =0.0507PUandXMR =0.091PU.–GivetheSQcage‘rotorunsaturatedmutual reactance’(XMR)thesamevalueastheWR ‘rotorleakagereactance’(XLR).
TheWoundRotor(WR)andSquirrelCage(SQ)InductionMachineModelsinthePSCAD®Library
Figure1 Circuitdiagram(WR–top,SQcage–bottom)
Figure2 SQcage(doublecage)equivalentcircuit
Figure3 WRIM(singlewinding)equivalentcircuit
TIN1
0.0
0.0 I M
W
S
T Motor
RRL
S
TL
I M W
TIN2 X 2
W *
0.2 TIN1
0
0
Timed Breaker Logic
Open@t0 BRK
BRK
X 2 W2
* 0.2
TIN2
RS
RC1
XLS
XLC2
RC2
XMR
XM
RS XLS
XLR
RR
XM
N O V E M B E R 2 0 0 9 7D E C E M B E R 2 0 1 1 7
Figure4showsthedataentryfortheSQcage(left)andWRmodels(right).Byusingequivalentvalues,bothmodelsshowcomparablebehaviour(Figure5)andrepresentasinglecagemachinedesign.
ThesimulationresultsshowninFigure5showthatthespeed(W–WR,W2–SQcage)andtorque(T–WR,T2–SQcage)ofbothmachinesareidentical.Thus,anyoneoftheinductionmachinemodelsmaybeusedtorepresentasinglecageinductionmachine.
Example2:Modelingadoublecageinductionmachine. TheWRmachinemodelcanbesetuptorepresentadoublecageSQcagemachine(IM_study_02.pscx).
IntheWRmodel,selectthe“No.ofRotorSquirrelCages=1”,asshowninFigure6.TheequivalentcircuitrepresentationisasinFigure7.
Figure4 SQcageandWRsetupconfiguration
Figure5 Simulationresults(IM_study_06_a.pscx)
Figure6 WRconfiguration
Simulation Results
time(s) 0.00 0.25 0.50 0.75 1.00 1.25 1.50 1.75 2.00
0.0
1.10
PU
W W2
-0.10
0.80
PU
Te Te2
Figure7 WRIM(No.ofrotorsquirrelcages=1)equivalentcircuit
RS
RR
RLR
XLS
XLC1
RC1
XMR
XM
8 P U L S E T H E M A N I T O B A H V D C R E S E A R C H C E N T R E J O U R N A L
Figure8showsthedataentryfortheWRmodel.Withtheappropriatedata,theSQcageandWRmachinemodelswillgiveidenticalresults(Figure9).
Conclusions Ascanbeseenfromtheresults,aSQcageandWRmachinemodeldeliverequivalentresultswhenconfiguredproperly.Hence,aSQcagemachinemodelcanbeaccuratelyrepresentedusingaWRmachinemodel.PSCAD® users are encouraged to use the WRIM model due to its more conventional and straight forward parameter configuration.
PSCAD®Cases:IM_study_01.pscxandIM_study_02.pscx
Figure8 WRsetupconfiguration
Figure9 Simulationresults(IM_study_06_b.pscx)
A SQ cage and WR machine model deliver equivalent results when configured properly…
D E C E M B E R 2 0 1 1 9
NewPTConnectionsDr. Namal Fernando, Manitoba Hydro
Background Generator and transformer protection upgrade at Seven Sisters generation station.Therearesixunitsandtheexistingelectromechanicalrelaysarebeingreplacedwithmulti-functionaldigitalrelays.Theprojectincludesreplacementoflineendpotentialtransformers;theexistingtwopotentialtransformers(i.e.opendeltawithphaseBgrounded)arebeingreplacedwiththreepotentialtransformers(groundedwye).Thereisonlyonesynchronizingsystemforallsixunits.Incomingvoltagereferenceislinevoltage;phaseABwithBatgroundpotential.
Problem Sincethenewdesignincludesthreepoten-tialtransformerswithneutralgrounded,wecouldnotconnectdirectlytotheexistingsynchronizersystem.TheexistingsystemisbasedonphaseBatgroundpotentialandcommontoalltheunits,whereastheunitswiththenewprotectiondesignwillhaveneutralpointgrounded(i.e.,forunitswithnewprotectiondesign,thephaseBisnolongeratgroundpotential).
Solution InstallanisolatingtransformerbetweenthelinevoltageABandtheincomingvoltageinputtothesynchronizersystem.
PSCAD®Application ItiswellknownthatPTsshouldbeconnectedincorrectphasesequence.Whilethecorrectconnectionscanbedeterminedthroughsimplehandcalculationsbyconstructingrelevantphasordiagrams(Figure1),thisisnotalwaysstraightforward.
Therearemanyinstanceswhereincorrectconnec-tionshavecausedunittrippingatthecommissioningandtestingstage.Thiscouldcreateaheadacheforallinvolvedandtheconsequencescanbesignificant.PSCAD®providesasimpleandefficientwaytoverifythenewconnections.WeusedasimplePSCAD®simulationcircuittoverifythatthePTconnectionscorrespondingtotherunningandincomingvoltagestothesynchronizerareconnectedproperly.
Ea
D
0.155559 30
Figure1 Phasordiagram
1 0 P U L S E T H E M A N I T O B A H V D C R E S E A R C H C E N T R E J O U R N A L1 0 P U L S E T H E M A N I T O B A H V D C R E S E A R C H C E N T R E J O U R N A L
ThePSCAD®caseusedforthestudyisshowninthefigurebelow.Thesimulationisnotcomplex.However,wefindthistobeausefulengineeringapplication.TheschematicdiagramsareshowninFigures2and3.
TheimportantdataforthissimulationisjustthePTvoltage(turns)ratios.Otherdetails,suchassaturation,etc.arenotimportantforthisbasicanalysis.
Figure2 NewPTconnection
Figure3 OldPTconnection
PUBLICATIONAGREEMENT#41197007RETURNUNDELIVERABLECANADIANADDRESSESTO
MANITOBAHVDCRESEARCHCENTRE211COMMERCEDRIVE
WINNIPEGMBR3P1A3CANADA
D E C E M B E R 2 0 1 1 1 1
JuanCarlosGarciaAlonso,P.Eng.Power System Simulation & Studies Engineer
JuanCarlos(JC)receivedhisElectricalEngineeringdegreefromtheNationalUniversityofColombia,Bogota,Colombiain1996andsubsequentlyreceivedhisM.Sc.degreefromtheUniversityofManitoba,Canada.HedesignedpowertransformerswithPauwelsTransformersinWinnipegandin2006joinedtheMHRC.JCparticipatesinvariousengineeringserviceprojectsintheareasofinsulationcoordination,VSCs,protectionandsuperconductivemagneticdevices,amongothers.HismainfocusduringthisperiodhasbeenwritingnewmodelsformagneticsimulationwithPSCAD®.
JCcanbefoundenjoyinghisfavouriteoutdooractivities,suchasrockclimbing,canoeingandhiking.
ArashDarbandiEngineering Application Specialist
ArashreceivedhisElectricalEngineeringdegreefromtheUniversityofManitoba,Canadain2010andiscurrentlypursuinghisM.Sc.atthesameuniversity.Inhisshorttimeherewithus,ArashhasimprovedthelinefeaturesoftwareofourIceVisionsystemanddevelopedanewalgorithmtoimprovetheexistingsoftware.ArashassistedwiththeLineFaultLocator(LFL)productbydevelopingnewfactoryacceptancetestsfortheLFL,improvingsoftwarequal-ityandperformance.Arashiscurrentlyinvolvedwiththebatteryre-purposingresearchprojectdevelopingapowerelectronicgridinterconnectionandareactivepowerstudy.Heisalsoperformingreactivepowerstudiesindifferentplants,aswellasprovidingrecommendationstoclientstoimprovetheirsystemperformance.
Arashenjoysahealthyandactivelifestyle,volunteeringwiththeUniversityofManitobaSatelliteteamastheirTechnicalCoordinator,andtravellinginternationallytoexperiencecultureandcuisine.
Manitoba HVDC Research Centre
MeettheTeam!
TheManitobaHVDCResearchCentrepridesitselfonitsexcellentcustomersupportandservice.Oursuccessisadirectresultofourclientfocusedefforts.Wearecommittedtoprovidingourclientswiththebestpossiblesupporttoensureoptimumsuccesswithourproductsandservices.“MeettheTeam”willbearegularlypublishedadditiontothePulseNewslettertointroduceourexperiencedteammembers.ThispublicationfeaturesJuanCarlosGarciaAlonsoandArashDarbandi;justafewofthedynamicstaffmemberswearefortunatetohaveattheManitobaHVDCResearchCentre(MHRC).
Puls
eis
dis
trib
ute
df
ree
of
char
ge
and
isp
ost
ede
lect
ron
ical
lya
tww
w.h
vdc.
caI
fyo
uw
ou
ldli
ket
or
ecei
vea
co
py
ofP
uls
e,p
leas
ese
nd
us
ane
mai
lto
info
@h
vdc.
caA
rtic
les
and
su
bm
issi
on
sad
dre
ssin
gt
he
use
of
PSC
AD
®in
th
ere
alw
orl
da
rea
lway
sw
elco
me.
©20
11M
anit
ob
aH
VD
CR
esea
rch
Cen
tre,
ad
ivis
ion
of
Man
ito
ba
Hyd
roIn
tern
atio
nal
Ltd
.Pr
inte
din
Can
ada
ExpandingKnowledgeThefollowingcoursesareavailable,aswellascustom training courses–[email protected].
FundamentalsofPSCAD®andApplicationsIncludesdiscussionofACtransients,faultandprotection,transformersaturation,windenergy,FACTS,distributedgeneration,andpowerqualitywithpracticalexamples. Duration: 3 Days
AdvancedTopicsinPSCAD®SimulationIncludescustomcomponentdesign,analysisofspecificsimulationmodels,HVDC/FACTS,distributedgeneration,machines,powerquality,etc. Duration: 2–4 Days
HVDCTheory&ControlsFundamentalsofHVDCTechnologyandapplicationsincludingcontrols,modelingandadvancedtopics. Duration: 4–5 Days
ACSwitchingStudyApplicationsinPSCAD®Fundamentalsofswitchingtransients,modelingissuesofpowersystemequipment,straycapacitances/inductances,surgearresterenergyrequirements,batchmodeprocessingandrelevantstandards,directconversionofPSS/EfilestoPSCAD®. Duration: 2–3 Days
DistributedGeneration&PowerQualityIncludeswindenergysystemmodeling,integrationtothegrid,powerqualityissues,andotherDGmethodssuchassolarPV,smalldieselplants,fuelcells. Duration: 3 Days
LightningCoordination&FastFrontStudiesSubstationmodelingforafastfrontstudy,representingstationequipment,straycapacitances,relevantstandards,transmissiontowermodelforflash-overstudies,surgearresterrepresentationanddata. Duration: 2 Days
MachineModelingincludingSRRInvestigationandApplicationsTopicsincludemachineequations,exciters,governors,etc.,initializationofthemachineanditscontrolstoaspecificloadflow.AlsodiscussedaretypicalapplicationsandSSRstudieswithseriescompensatedlinesasthebasecase. Duration: 2 Days
ModelingandApplicationofFACTSDevicesFundamentalsofsolid-stateFACTSsystems.Systemmodeling,controlsystemmodeling,convertermodeling,andsystemimpactstudies. Duration: 2–3 Days
TransmissionLines&ApplicationsinPSCAD®
Modelingoftransmissionlinesintypicalpowersystemstudies.Historyandfundamentalsoftransmissionlinemodeling,discussiononmodels,suchasPhase,Modal,BergeronandPIintermsofaccuracy,typicalapplications,limitations,etc.,examplecasesanddiscussionontranspo-sition,standardconductors,treatmentsofgroundwire,cross-bondingofcables,etc. Duration: 3 Days
WindPowerModelingandSimulationusingPSCAD®
Includeswindmodels,aero-dynamicmodels,machines,softstartinganddoublyfedconnections,crowbarprotection,lowvoltageridethroughcapability. Duration: 3 Days
ConnectwithUs!January11–13,20122012PSCAD®andRTDSAsiaConferencewww.nayakpower.comBangalore,India
January18–22,2012Elecrama–2012www.elecrama.com/elecrama2012/index.aspxMumbai,India
January24–26,2012DistribuTECHConference&Exhibitionwww.distributech.com/index.htmlSanAntonio,Texas,USA|Booth#4541
March27–30,20122012PSCADEuropeanUserGroupMeetingtraining@pscad.comCastelldefels,Spain
June3–6,2012AWEAWindpower2012Conference&Exhibitionwww.windpowerexpo.orgAtlanta,Georgia,USA|Booth#7513
August27–31,2012CIGRESession44andTechnicalExhibitionwww.cigre.org/gb/events/sessions.aspParis,France
Moreeventsareplanned!Pleaseseewww.pscad.comformoreinformation.
PSCAD® Training Sessions
Hereareafewofthetrainingcoursescurrentlyscheduled.Additionalopportunitieswillbeaddedperiodically,sopleaseseewww.pscad.comformoreinformationaboutcourseavailability.
April17–19,2012FundamentalsofPSCAD®andApplications
May15–17,2012HVDCTheoryandControls
September11–13,2012FundamentalsofPSCAD®andApplications
September18–20,2012WindPowerModeling&SimulationusingPSCAD®
November27–29,2012HVDCTheoryandControls
AlltrainingcoursesmentionedaboveareheldattheManitobaHVDCResearchCentreInc.Winnipeg,Manitoba,[email protected] www.pscad.com
PleasevisitNayakCorporation'swebsitewww.nayakcorp.comforcoursesintheUSA.
For more information on dates, contact [email protected] today!