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8/6/2019 Voltage induced in a single phase
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VoltageinducedinasinglephaseTherotorinthegeneratorillustratedaboveproducesafluxwhichpassesradiallyfromtherotorsurfaceintothestator.Thecircumferentialvariationofthisradialfluxdensityaroundtherotorcanbedescribedusing
whereistheanglearoundthesurface.Iftherotorofthemachinerotatesatcon
stantspeedtthenthefluxdensityseenataposition0onthestatorwillbegivenby
Usingthegeneratorlaw
thevoltageinducedineachsideofthecoilcanbeobtained.Consideringtheconductorat0=0,thevelocityoftheconductorwithrespecttothefluxisdown(thefluxdensityismovinguprelativetotheconductor),thefluxdensityislefttoright,thecrossproductisparallelwiththeconductor.Ifwetaketheconductortobeorientedwithpositvedirectionoutofthepagethentheinducedvol
tageisgivenby
Relatinglinearvelocitytoangularvelocity
theinducedvoltagebecomes
Forthereturnsideoftheconductorat0=,
Therfore,thetotalvoltageinducedintheloopformedbythetwoconductorsis
Now,ifthereareNTloopsformingacoil,
Notingthattheareaenclosedbythecoilisgivenby2rlthevoltagecanalsobewrittenas
Amulti-coilmachineInthesimpleexamplewithonlyonecoil,thereisasignificantwasteofspace
inthemachine.Itispossibletoaddadditionalcoilstothestatorandmakefulluseoftheavailablespace.IfthereareNcoilscoils,allcapableofcarryingequalcurrent,Ithemaximumavailablepowerisgivenby
.Unfortunately,toaccessthispower,eachcoilwouldneedtobeconnectedtoaloadbyitsowntransmissionline.Thisisunacceptablyexpensiveforatransmissionanddistributionsystem.Asanalternative,allthecoilscouldbeconnectedtogtetherinseriestoformasinglephasevoltage.Ifallthecoilsareconnectedinseriesthetotalavailablevoltageisgivenbythephasorsummationoftheindividalcoilvoltages:
andtheavailablepoweris
8/6/2019 Voltage induced in a single phase
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InthecasewhereNcoilsislarge,theseriesconnectedpoweris2/timestheavailblemaxiumumpower(about64%).
AThree-phasemachineClearlysomecompromisebetweengeneratorutilizationandpowerdeliverycostmustbereached.Thiscompromiseisthethree-phasepowersystem.Inathree-phase
generator,therearestillmanycoilsinthemachine,butthecoilsarenowconnectedinthreedistinctgroups,calledphases.Notingthatthesumofallthecoilvoltagesmustequalthesumofthephases,thermsphasevoltagecanbeobtained:
Now,ifeachphaseisconnectedtoaloadbyitsowntransmissionline,thetotalavailablepowerisgivenby
andifthenumberofcoilsislarge:
General3-phasevoltagesIngeneralinthecoursewewillthinkofathree-phasewindingasbeingmadeupofonlythreecoils,separatedby120degrees.However,itisimportanttorealisethatarealmachinehasmanycoilswhicharegroupedintothreephases.Asshownabove,thefundamentalvoltageinducedinaphasecomprisedofanumberofdistributedcoilswillbeslightlylowerthanthatproducedbyasinglecoilwiththesametotalnumberofturns.Distributedwindingscanalsoreducethemagnitudeofhigherharmonicswhichmaybeinducedinacoil.Detailedinfomrationaboutdistributedwindingsisbeyondthescopeofthecourse,moreinformationcanbefoundintheappendicesofthetextbook.