正弦量的向量表示法課件講解

VectorRepresentationofSinusoidalQuantities正弦量的向量表示法運(yùn)用復(fù)數(shù)分析電路的方法稱為相量法(phasormethod)。Themethodofusingcomplexnumberstoanalyzecircuitsisreferredtoasthephasormethod.1.復(fù)數(shù)ComplexNumbers設(shè)一個(gè)復(fù)數(shù)A=a+jb，其中a、b都是實(shí)數(shù)，a為復(fù)數(shù)的實(shí)部，b為復(fù)數(shù)的虛部，為虛數(shù)單位(虛數(shù)單位在數(shù)學(xué)中用i表示，因電工學(xué)中用i表示電流，故改用j以示區(qū)別)。ConsideracomplexnumberA=a+jb,wherebothaandbarerealnumbers.Here,aistherealpart,bistheimaginarypart,andistheimaginaryunit(oftenrepresentedasjinelectricalengineeringtoavoidconfusionwiththesymboliusedforcurrentinmathematics).例如，3+j4對應(yīng)于圖中復(fù)平面上的P1點(diǎn)。Forexample,3+j4correspondstothepointP1inthecomplexplane,asillustratedinfollowingfigure.復(fù)平面complexplaneRealAxis復(fù)數(shù)還可以用復(fù)平面上的一個(gè)矢量來表示。Complexnumberscanalsoberepresentedbyavectorinthecomplexplane.如A=3+j4可以用一個(gè)從原點(diǎn)O到P點(diǎn)的矢量來表示。Forinstance,A=3+j4canberepresentedbyavectorOPfromtheoriginOtothepointP.這種矢量稱為復(fù)數(shù)矢量。Thistypeofvectoriscalledacomplexvector.復(fù)平面中的矢量vectorinthecomplexplane矢量與實(shí)軸正方向的夾角θ稱為復(fù)數(shù)A的輻角。TheangleθbetweenthevectorandthepositiverealaxisistermedtheargumentofthecomplexnumberA.RealAxis任意一個(gè)復(fù)數(shù)A可對應(yīng)一個(gè)復(fù)數(shù)矢量OP，如圖所示。AnycomplexnumberAcorrespondstoacomplexvectorOP,asshowninthediagram.矢量的長度定義為復(fù)數(shù)A的絕對值，稱為復(fù)數(shù)的模。即ThelengthofthevectorisdefinedastheabsolutevalueofthecomplexnumberA,knownasthemodulusofthecomplexnumber,denotedas因?yàn)锽ecause根據(jù)歐拉公式BasedonEuler'sformula(1)式(1)又可以寫為Equation(1)canberewrittenas復(fù)平面中的矢量vectorinthecomplexplaneRealAxis復(fù)數(shù)的四則運(yùn)算規(guī)則如下Therulesforthefourfundamentaloperationswithcomplexnumbersareasfollows.設(shè)Set則Then設(shè)有時(shí)間t的復(fù)值函數(shù)，利用數(shù)學(xué)中的歐拉公式Consideracomplex-valuedfunctionoftimet,utilizingEuler'sformulainmathematics：ej

t=cos

t+jsin

t

顯然Obviouslycos

t=Re(ej

t)sin

t=Im(ej

t)這里，Re(·)和Im(·)分別為取實(shí)部和取虛部的符號。進(jìn)一步，有Here,Re(·)andIm(·)representthesymbolsfortakingtherealandimaginaryparts,respectively.Furthermore,wehave:Imej(

t+

)=Imcos(

t+

)

+jImsin(

t+

)2.用相量表示正弦量RepresentationofSinusoidalQuantitiesUsingPhasors顯然正弦電流i(t)＝Imsin(

t+

)可以表示為Clearly,thesinusoidalcurrenti(t)=Imsin(t+

)canbeexpressedasi(t)＝Im[Imej(

t+

)]=Im[Imej

ej

t]Imej(

t+

)稱為復(fù)指數(shù)電流。記復(fù)數(shù)電流Imej(t+)isreferredtoasthecomplexexponentialcurrent.Denotethecomplexcurrentas:

式中，Im為的模，則WhereImisthemagnitudeof,then

i(t)＝Im

[]2.用相量表示正弦量RepresentationofSinusoidalQuantitiesUsingPhasors在電路中，通常把電流的振幅（或有效值）與其初相角構(gòu)成的一個(gè)復(fù)數(shù)稱為電流相量。例如Incircuits,theamplitude(oreffectivevalue)ofacurrent,alongwithitsinitialphaseangle,isoftenreferredtoasacurrentphasor.Forinstance,i(t)＝5sin(

t

30

)A對應(yīng)電流相量為Thecorrespondingcurrentphasoris（最大值相量Themaximumvaluephasor）（有效值相量TheEffectivevaluephasor）2.用相量表示正弦量RepresentationofSinusoidalQuantitiesUsingPhasors類似地，若有電壓Similarly,ifthereisavoltageas

u(t)＝10sin(

t+50

)V電壓相量為thenthevoltagephasoris

（最大值相量Themaximumvaluephasor）若用有效值為相量的模，則有效值相量為Ifweusetheeffectivevalueasthemagnitudeofthephasor,theeffectivevaluephasoris:

（有效值相量TheEffectivevaluephasor）2.用相量表示正弦量RepresentationofSinusoidalQuantitiesUsingPhasors正弦量用相量表示后，還可以用相量圖來表示。Afterrepresentingsinusoidalquantitiesusingphasors,theycanalsobedepictedusingphasordiagrams.設(shè)電流相量Letthecurrentphasequantity它們的相量圖如下圖所示Theirphasordiagramsareshownbelow二者之和按平行四邊形