直流电机毕业论文中英文资料对照外文翻译文献.docx
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IntroductiontoD.C.Machines
D.C.machinesarecharacterizedbytheir versatility.Bymeansofvariouscombinationsofshunt-,series-,andseparatelyexcitedfieldwindingstheycanbedesignedtodisplayawidevarietyofvolt-ampereorspeed-torquecharacteristicsforbothdynamicandsteadystateoperation.Becauseoftheeasewithwhichtheycanbecontrolled,systemsofD.C.machinesareoftenusedinapplicationsrequiringawiderangeofmotorspeedsorprecisecontrolofmotoroutput.
TheessentialfeaturesofaD.C.machineareshownschematically.Thestatorhassalientpolesandisexcitedbyoneormorefieldcoils.Theair-gapfluxdistributioncreatedbythefieldwindingissymmetricalaboutthecenterlineofthefieldpoles.Thisiscalledthefieldaxisordirectaxis.
Asweknow,theA.C.voltagegeneratedineachrotatingarmaturecoilisconvertedtoD.C.intheexternalarmatureterminalsbymeansofarotatingcommutatorandstationarybrushestowhichthearmatureleadsareconnected.Thecommutator-brushcombinationformsamechanicalrectifier,resultinginaD.C.armaturevoltageaswellasanarmaturem.m.f.Wavethenis90electricaldegreesfromtheaxisofthefieldpoles,i.e.inthequadratureaxis.Intheschematicrepresentationthebrushesareshowninquadratureaxisbecausethisisthepositionofthecoilstowhichtheyareconnected. Thearmaturem.m.f.Wavethenisalongthebrushaxisasshown.(Thegeometricalpositionofthebrushesinanactualmachineisapproximately90electricaldegreesfromtheirpositionintheschematicdiagrambecauseoftheshapeoftheendconnectionstothecommutator.)
Themagnetictorqueandthespeedvoltageappearingatthebrushesareindependentofthespatialwaveformofthefluxdistribution;forconvenienceweshallcontinuetoassumeasinusoidalflux-densitywaveintheairgap. Thetorquecanthenbefoundfromthemagneticfieldviewpoint.
Thetorquecanbeexpressedintermsoftheinteractionofthedirect-axisair-gapfluxperpole andspace-fundamentalcomponent ofthearmaturem.m.f.wave.Withthebrushesinthequadratureaxistheanglebetweenthesefieldsis90electricaldegrees,anditssineequalsunity.Fora polemachine
(1-1)
Inwhichtheminussigngasbeendroppedbecausethepositivedirectionofthetorquecanbedeterminedfromphysicalreasoning.Thespacefundamental ofthesawtootharmaturem.m.f.waveis timesitspeak. Substitutioninaboveequationthengives
(1-2)
Where, =currentinexternalarmaturecircuit;
=totalnumberofconductorsinarmaturewinding;
=numberofparallelpathsthroughwinding.
And
(1-3)
is aconstantfixedbythedesignofthewinding.
Therectifiedvoltagegeneratedinthearmaturehasalreadybeendiscussedbeforeforanelementarysingle-coilarmature.Theeffectofdistributingthewindinginseveralslotsisshowninfigure.Inwhicheachoftherectifiedsinewaveisthevoltagegeneratedinoneofthecoils,commutationtakingplaceatthemomentwhenthecoilsidesareintheneutralzone.Thegeneratedvoltageasobservedfromthebrushesandisthesumoftherectifiedvoltagesofallthecoilsinseriesbetweenbrushesandisshownbytheripplinglinelabeled infigure.Withadozenorsocommutatorsegmentsperpole,theripplebecomesverysmallandtheaveragegeneratedvoltageobservedfromthebrushesequalsthesumoftheaveragevaluesoftherectifiedcoilvoltages.Therectifiedvoltage betweenbrushes,Knownalsoasthespeedvoltage,is
(1-4)
where isthedesignconstant.Therectifiedvoltageofadistributedwindinghasthesameaveragevalueasthatofaconcentratedcoil.Thedifferenceisthattherippleisgreatlyreduced.
Fromtheaboveequations,withallvariableexpressedinSIunits,
(1-5)
Thisequationsimplysaysthattheinstantaneouspowerassociatedwiththespeedvoltageequalstheinstantaneousmechanicalpowerwiththemagnetictorque.Thedirectionofpowerflowbeingdeterminedbywhetherthemachineisactingasamotororgenerator.
Thedirect-axisair-gapfluxisproducedbythecombinedm.m.f. of the fieldwindings. Theflux-m.m.f.Characteristicbeingthemagnetizationcurvefortheparticularirongeometryofthemachine. Inthemagnetizationcurve,itisassumedthatthearmature–m.m.f. Waveisperpendiculartothefieldaxis.Itwillbenecessarytoreexaminethisassumptionlaterinthischapter,wheretheeffectsofsaturationareinvestigatedmorethoroughly.Becausethearmaturee.m.f.isproportionaltofluxtimesspeed,itisusuallymoreconvenienttoexpressthemagnetizationcurveintermsofthearmaturee.m.f. ataconstantspeed .Thevoltage foragivenfluxatanyotherspeed isproportionaltothespeed,i.e.
(1-6)
Thereisthemagnetizationcurvewithonlyone