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Design&AnalysisforElectronicMachineSystemInstituteofPowerElectronicsandMotorControlTsinghuaUniversityZhengmingZhaoFeb.18,20011ChapterOne:Introduction1-1EvolutionofACElectricMachines1.DevelopmentofACelectricmachines
*Whatistheelectricmachine?
DeviceforelectromagneticconversionsTheoreticalbase:Maxwellelectromagnetictheory
(1850s)2MagneticsElectricityGeneratorElectricityMagneticsMotorElectricityMagneticsElectricityTransformerThreedevelopingways:
(1)DesignYearWeightCost
(p./hp)
(US$/hp)1890200180195722221976101019905.24.6*Reduced40times3(2)ModelingandSolution:1880-1910s:Classicalanalyticalelectromagneticfield1920s-1960s:Electricalcircuit--Park’sequation(double-axis)1970s-1980s:Numericalmethodforfieldequations(finiteelementanalysis,ANSYS)1980s-present:Combinationoffieldandcircuit
(3)ConstructionandMode:InductionSynchronousPMbrushlessDCSwitchedreluctance
4PMAxially-LaminatedSynchronousReluctanceMachine*Highpowerdensity*Highefficiencyandpowerfactor*Widespeedrange*Highreliability5PermanentMagnetMachines*Highefficiency*Highpowerfactor*Highreliability*Structurediversity6SwitchedReluctanceMachines*Highefficiency*Highfaulttolerance*Widespeedrange*Simplestructure7SwitchedReluctanceMachines8Cross-SectionofAnInductionMachine91-2WhatistheElectronicMachine?PowerSupplyElectricMachineLoadControllerElectronicMachineFourdevelopingtrends:*Integration:powerelectronics*Intelligence:fuzzy,neuro-network*Universal:universalmachinesystem*Information:communication,DSP,wireless101-3TheApplicationsofElectronicMachines*Lessthan3%inapplicationsDomesticApplicationsIndustrialApplicationsTraction/AutomotiveDefense/AerospaceApplicationsCommercialApplicationUtilityApplicationsIncreasingpower11ChapterTwo:GeneralandSpecialDesignFeaturesofElectronicMachines2.1DifferencesofElectronicandConventionalMachines12
MechanicalCharacteristicsofInductionMachineFivekeypoints:(1)RatedtorqueTn(2)StartingtorqueTs(3)MaximumtorqueTm(4)Stabilityarea(5)InstabilityareaTmTsTnInstabilityareaABC13MinimumSlipandMaximumEfficiency*Comparisonforthreetorque-speedcurvesasdifferentsupplyfrequencyandvoltage*Lossesandefficiencycurves14WithoutvectorcontrolWithvectorcontrolVectorControlforMotorDrive*D-axis:magnetizingaxis;Q-axis:torqueaxis*Constantfluxdensity*Idsforwholemagnetizingfield*Ir=IqrandIdr=015TypicalInverter-drivenInductionMotorSystemSwitch(IGBT)RectifierPWMController
InductionMotorLoadTrianglecarrierSinusoidalReference16Pulse-Width-Modulation(PWM)andHarmonics*Vref>Vtri,switchison*Vref<Vtri,switchisoff*Thefundamentalcomponentof
theoutputphasevoltageissinusoidalbase*Therearelotsofharmonics
1718QuestionandDiscussion1.What’stheelectronic
machinesystem?2.Whataredifferencesbetweentheelectronicandconventionalmachines?192.2DesignFreedomandStrategies(1)ConventionalDesignStrategiesa.Fulfillneededstart-upcharacteristics(50%)Requirements: *Limitinrushcurrent *Generatehighstartingtorque *Ensurehighstartingefficiency *Eliminateharmonicsb.Provideappropriatesteadystatecharacteristics(efficiency,powerfactor,andsoon)(30%)c.Permiteasyandeconomicproduction(20%)20(2)Inverter-drivenDesignStrategiesa.Twofreedoms:*Completelyabandonstart-upcurrent,torqueandefficiencywith
fixedfrequency*Don’tcareabnormalharmonicstorqueatthetimeofstartingb.Threevaluablebenefits:*Maximumefficiencyandimprovedpowerfactorareintroducedintosizingequation*Theshapeofrotorslotcanbemostsuitabledesigned*Theconstraintconditionsofmatchofstatorandrotorslotnumber
canbeeliminated21DesignofmaindimensionsSelectionofairgaplengthStatorwindingsdesignStatorslotdesignstatorouterdiameter
RotorwindingsdesignRotorslotdesignRotorinnerdiameterFluxdensityLinecurrentdensityL/Di1RelatedparameterswithstatorcurrentdensityRelatedparameterwithstatorfluxdensityRelatedparameterswithstatorcurrentdensityRelatedparameterwithstatorfluxdensityMachineDesignFlowChart222.3SizingEquationforMachineDesign2.3.1SizingequationforconventionalmachinedesignFiveequations:
(1)Back-emfequation:(2)Outputpowerequation:(3)Fluxequation:(4)Surfacecurrentdensityequation:(5)Polepitchequation:23Dil:statorinteiraldiameterL:effectivelengthofstatorBg:
fluxdensityinairgapP:
ratedoutputpowerns:ratedspeedC:
machineconstant:efficiencycos:ratedpowerfactorKe:
back-emfcoefficientKw:
windingcoefficientA:surfacecurrentdensityConventionalSizingEquation242.3.2SizingEquationforElectronicMachines(1)Frequencyequation:Statorcurrentdensityequation:Slotareaofstator:Roundslotarea:25SizingEquationforElectronicMachines(2)Fluxdensityequationsinparts:FluxdensityinairgapFluxdensityinteethFluxdensityincoreKs:fluxcoefficient26SizingEquationforElectronicMachines(3)Ratioofareasincopperandslot:27SizingEquationforElectronicMachines(4)Statorslotarea:28SizingEquationforElectronicMachines(5)29SizingEquationforElectronicMachines(6)Finalsizingequation:Features:(1)Outerdiameterasvariable(2)Outputfunctioninsteadof
machineconstantCurvesfordifferenta,bandc30HomeworkI
Fromthefollowingequations,
Derivetheequation:Andexplainitsphysicalmeaning.and31RotorSlotDesign1.RotorslotshapeThreekeypoints:slotshape,slotnumber,slotdimensionsTwomainslotshapes:
RoundbottomFlatbottom32
Rotorshapeforconventionalinductionmotor*Itiscommontoadoptadoublecageordeepbarstoincreasetheskineffectforlargerotorresistanceduringstartingandhighstartingtorque.DoublecageDeepbarStartingtorque(s=1):33
rb:nominalrotorresistancewithoutconsiderationofskineffect
lb:lengthoftherotorconductorle:effectivelengthoftherotorcore
kr:acoefficientaccountingforskineffecthb:theheightofrotorconductorbb:thewidthofrotorconductorbr:thewidthofrotorslotSF:slipfrequency
r:rotorconductorconductivityEffectiveRotorResistance
34RotorSlotLeakageReactance*Therelationoftherotorslotleakagepermeance
rtotheshapeof
therotorslotfeaturedbyh/b2andb1/b2isshownastheFig.*Adeepslot(h/b2>2)withatip-uptriangularshape(b1/b2<0.6)
hasaverylargerandincreasestherotorleakagereactance.*Withoutconsiderationsofthe
startingcharacteristics,therotor
slotcanbewiderandshorter(h/b2<1.5andb1/b2>0.9)
underthelimitationoftheflux
densityinrotorteeth.35*Thisresultsinamuchreducedrotorleak
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