Example: air traffic controller

Chapter 14

Chapter14 MODULATIONINTRODUCTIONA swehaveseeninpreviousthreechapters, ,thesourceinformationisimpresseduponacar rier-wave(essentiallyasinusoidofacertain frequency) ( ,audio,voltagepulsetraincarryingdigitali nformation) forexample,therepresentationofsampledsig nalsbytheamplitude, (2,6,9)thatwecanwritethissinusoidalcarri ersignalas:c(t)=Acos(2 fct+ )( )Here,Aiscalledtheamplitudeand ,dataareusedtomodulateorchangeitsamplitu de,frequency, , (digitalmodulation) ,wealsodescribeaspecialcaseofdigitalmodu lationthatisveryimportantfortransmission ofinformationusingmodems quadratureamplitudemodulation(QAM) atechniquecalled675676 ThePhysicalLayerofCommunicationsSystemso rthogonalfrequencydivisionmultiplexing(O FDM). , , (smallerwavelengths) , , ,thistimetoanintermediatefrequency(IF) (multiplexing). , ,thecharacteristicsofthemodulatedsinusoi d(suchasamplitude,frequencyorphase) (AM)andfrequencymodulation(FM) , , , EncoderChannel EncoderModulatorChannelDe-modulatorChann el DecoderSource [1].

Section 14.2. In particular, we discuss amplitude and frequency modulation. We discuss discrete changes in the characteristics of the carrier (digital modulation) in 14.3 along with the methods of representing and analyzing the performance of these modulation schemes. We consider binary modulation schemes and multi-level modulation schemes here ...

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Transcription of Chapter 14

1 Chapter14 MODULATIONINTRODUCTIONA swehaveseeninpreviousthreechapters, ,thesourceinformationisimpresseduponacar rier-wave(essentiallyasinusoidofacertain frequency) ( ,audio,voltagepulsetraincarryingdigitali nformation) forexample,therepresentationofsampledsig nalsbytheamplitude, (2,6,9)thatwecanwritethissinusoidalcarri ersignalas:c(t)=Acos(2 fct+ )( )Here,Aiscalledtheamplitudeand ,dataareusedtomodulateorchangeitsamplitu de,frequency, , (digitalmodulation) ,wealsodescribeaspecialcaseofdigitalmodu lationthatisveryimportantfortransmission ofinformationusingmodems quadratureamplitudemodulation(QAM) atechniquecalled675676 ThePhysicalLayerofCommunicationsSystemso rthogonalfrequencydivisionmultiplexing(O FDM). , , (smallerwavelengths) , , ,thistimetoanintermediatefrequency(IF) (multiplexing). , ,thecharacteristicsofthemodulatedsinusoi d(suchasamplitude,frequencyorphase) (AM)andfrequencymodulation(FM) , , , EncoderChannel EncoderModulatorChannelDe-modulatorChann el DecoderSource [1].

2 ! ! , , , , (1G)oranalogcellularsystemsintheUSA, ,webrieflyconsideredamodelofadigitalcomm unicationsystemwherewehaveasource,asourc eencoder,andachannelencoderonthetransmit tersideandthecorrespondingchanneldecoder , , , ,ifthealphabetisbinary,thetwopossiblesym bolsare0and1andinformationissimplyalongs equenceof0 sand1 binary digitalsignalrepresentsthe zerosymbol usingaspecificsignalthatlastsforaduratio nofTssecondsandthe onesymbol , , ,mostsystemsareconstructedsuchthatM= , ,ifm1,m2,m3,andm4arethesymbolsofa4-arysy stem,wecanassociatethe dibit 00tom1,01tom2, (expressedinunitsofbaud).Thebitrate(ifM= 2k) s,thenthesymbolrateis1 (k=4oritisaM=16-aryalphabet) ,themessageismappedtotheamplitude,freque ncy,phase(oracombinationofthese) , , , , , (QAM).Inanalogmodulationwewereinterested intheSNR,butrecallfromChapter10thatindig italmodulationweareinterstedinthebiterro rrate(BER)asafunctionoftheratiooftheener gyperbit(Eb)tothevalueofthenoisePSD(N0) ,likeanalogmodulationwewouldliketomaximi zetheefficiencywithwhichweusetheavailabl ebandwidthindigitalmodulationwequantifyt hespectralefficiencyfortheamountofbandwi dthWrequiredtotransmitatagivendatarateRq uantifiedas = , ,therearetradeoffsbetweentheBERforagiven EbN0and.

3 690 ThePhysicalLayerofCommunicationsSystemst imetimeAmplitudeAmplitude100% Depth50% Depth0timeAmplitudetimeAmplitude10010010 0100 BasebandBasebandTS2TS3 , signalconstellation. Withasignalconstellation, ,thealphabethastwovalues 0 and 1. InASK,a 0 ismappedtooneamplitudevalueanda 1 ,a 0 ismappedtoonefrequencyvalueanda 1 ,a 0 ismappedtoonephasevalueanda 1 , (BASK).InBASK, ,si(t)=Aicos(2 fct+ ),0 t Tsfori=1,2( )Thetransmitterwilltransmits1(t)whentheb itiszeroands2(t) ,werefertothemodulationschemeashaving100 % (wherethetwoamplitudevaluesareAand0) ,wesaythatthemodulationdepthis50%. , zero bitisgivenby:Ezero= Ts0s21(t)dt=A21 Ts0cos2(2 fct+ )dt=A212 Ts0[1+cos(2 (2 fc)t+2 )]dt A212Ts( )Theapproximationisanequalityiffc=kTsand isacloseapproximationiffc$ one bitissimilarlyequalto:Eone=A222Ts( )Theaverageenergyperbitisgivenby:Eb,av=T s4[A21+A22]( )Hereweassumethatthenumberof 0 sandthenumberof 1 ,theaverageenergyperbitcanbecalculatedto beEb=A2Ts4andEb= , ( ).

4 Thebasebandsignalcanberecoveredattherece iverusingthesametechniquesasAM(enveloped etectionorcoherentdetection). , , someexamplesaretelevisionremotes, (BFSK).InBFSK, ,si(t)=Acos(2 fit),0 t Tsfori=1,2( ) (t)whenthebitiszeroands2(t) (t)ands2(t)whichinvolvesmultiplicationof thetwosignalsandintegrationoveronesymbol periodgivenby: Ts0s1(t)s2(t)dt=A2 Ts0cos(2 f1t)cos(2 f2t)dt=A22 Ts0[cos(2 (f1 f2)t)+cos(2 (f1+f2)t)]dt( )Theterm cos(2 (f1+f2)t) cos(2 (f1 f2)t) ,orthogonalFSKensuresthatthereisnocorrel ationbetweens1(t)ands2(t),thatis: Ts0s1(t)s2(t)dt=0( )InthecaseoforthogonalFSK,f1 f2=1 Tssothattheintegrationin cos(2 (f1 f2)t) (OFDM)lateroninthischapter( ).AswesawinthecaseofBASK,theenergyperbit inBFSK(forbotha 0 anda 1 ) , , ,anFSKsignal,likeFM, (Chapter10).RecallthataManchesterpulseco nsistsoftwo half (liketheAdvancedMobilePhoneSystem AMPS).Recently,FSKhasfoundapplicationsin lowpowerwirelessnetworkslikeBluetooth, (BPSK).

5 InBPSK, ,si(t)=Acos(2 fct+ i),0 t Tsfori=1,2( )Thetransmitterwilltransmits1(t)whentheb itiszeroands2(t) radians,themaximumpossiblephasedifferenc ebetweenthetwobitsis .Itiscommontoassumethat 1=0and 2= inwhichcase,thetwosignalswillbe:s1(t)=Ac os(2 fct),0 t Tss2(t)=cos(2 fct+ )= Acos(2 fct),0 t Ts( ) ,wecanseethatthereisareversalofphasewhen thebitchangesandso, (t)= s2(t)andwecanviewBPSKasBASK whereA1=AandA2= , ,BPSK isequivalenttoantipodalorbipolarsignalin gwithnon-return-to-zero(NRZ) , ,BPSK signals,likephasemodulation, , , ,althoughdifferentmodulationschemesareus eddependingonthetransmissionrate, dualBPSK fortransmissionsfromthecellphonetowertom obiledevices(downlink).Here,therearetwoB PSK signals, ,thesourceproducesoneofMsymbolsmifori=1, 2,3, , (t) , :si(t)=Aicos(2 fct+ ),0 t Tsfori=1,2,3, ,M( ) (2i 1 M) , , (inthiscased) 3, 1, :s1(t)=cos(2 fct+ ),0 t Tss2(t)= cos(2 fct+ ),0 t Tss3(t)=3cos(2 fct+ ),0 t Tss4(t)= 3cos(2 fct+ ),0 t TsNotethatonceagain, , :si(t)=Acos[2 fct+2 (i M2)!]

6 Ft],0 t Tsfori=1,2,3, ,M( )TheMfrequencieswillbefc+(i M2)!ffori=1,2,3, , ! , :si(t)=Acos(2 fct+ i),0 t Tsfori=1,2,3, ,M( )Thephase iistypicallygivenby i=2 M(i 1)+ (CDMA anddigitalTDMAinNorthAmerica). , 2, ,3 4,thefourphaseswillbe 4,3 4,5 4and7 4-QPSK,avariationofQPSK,thesymbolsarepic kedalternativelyfromthesetwoschemes(cons tant=0andconstant= 4) (multiplepositiveandnegative)amplitudesa reusedwiththetwophase-shiftedcarriers,th emodulationschemeiscalledquadratureampli tudemodulation(QAM). :si(t)=Ai,Icos(2 fct)+Ai,Qsin(2 fct),0 t Tsfori=1,2,3, ,M( ) :si(t)=Aicos(2 fct+ i),0 t Tsfori=1,2,3, ,M( )696 ThePhysicalLayerofCommunicationsSystemsw hereAi= A2i,I+A2i,Qand i= tan 1(Ai,QAi,I).Soitispossibleforustothinkof QAMasamixofbothamplitudeandphaseshiftkey ingsincethemessagemiismappedtoacarrierwi thamplitudeAiandphase ,itiscommoninM-QAMtopickthein-phaseandqu adrature-phaseamplitudessuchthattheyareo ftheform(2i 1 M) , ,recently, , , [1],[2].

7 Inmostcases,weassumethatthereceivedsigna lisonlycorruptedbyadditivewhiteGaussiann oise(AWGN) (t)forsomei 1,2,3, ,M,thereceivedsignalwillbe:r(t)=si(t)+n( t),0 t Ts( )Thegoalofthereceiveristodeterminewhatsi (t)wastransmittedgiventhatr(t) (t)was, ,r(t)iscorruptedbynoiseanditispossibleth atthereceiverwillsometimesdeterminethatt hetransmittedsignalwassj(t)wherej(=iwhen si(t) (Eb) (100% modulation ) 0 andabit 1. ,eventhevisualdifferencebetweenthe 0 bitandthe 1 ,whoafteralldonotsensevoltagesthatwell:- ).Asthereceivedsignalgetsnoisier, Tx signal with two bitsBASK Rx signalBASK Rx signalBASK Rx signalBASK Rx signalBASK Tx signal with two Rx signalBASK Rx signalEb/N0=10dBEb/N0=7dBEb/N0= :r(t)=Aicos(2 fct)+n(t),0 t Ts( )TorecoverthenumberAi, (a).Thatis,thereceivercomputes:Z= Ts0r(t)cos(2 fct)dt= Ts0 Aicos2(2 fct)dt+ Ts0n(t)cos(2 fct)dt=Ai2+ Ts0n(t)cos(2 fct)dt=Ai2+n( )wheren= Ts0n(t)cos(2 fct)dtisaGaussianrandomvariable(withzero meanandavariancethatisafunctionofN02) with threshold(a) BASK/BPSK receiverCompare with thresholds(a) MPSK/QAM receiverr(t)cos(2 fct)sin(2 fct)ZZ1Z2Ts0 TsTs00r(t)cos(2 fct) , ,undernoise-freeconditions, , 0 whena 1 ,fromacommonsenseperspective,ifZisaboveA i4,thereceiverdecidesthata 0 wastransmittedanda 1 , ,thereceiverneedstodetectwhetherthephase is0 or180.

8 Asimplewayofdeterminingthiswouldbetoperf ormthefollowingcomputation:Z= Ts0r(t)cos(2 fct)dt( ) ,thecomputednumberZwillbeasfollows:Z={A Ts0cos2(2 fct)dt+ Ts0n(t)cos(2 fct)dtifthephaseis0 A Ts0cos2(2 fct)dt+ Ts0n(t)cos(2 fct)dtifthephaseis180 ( )MODULATION699 Notethatinthenoiselesscase(n(t)=0),Zwill havealargepositivevalue(A2)whenthephasei s0 andalargenegativevalue( A2)whenthephaseis180 . ,thereceiverdecidesthatthe 0 bitwastransmittedifZispositiveandthe 1 ( ). ,thevalueofZmaybemovedtowardszeroandinso mecases, , :r(t)=Acos(2 fct+ i)+n(t)( ) ,thereceiverwillmultiplythereceivedsigna lbybothasineandacosinecarrier(thatareloc allygenerated) (b). :Z1=A Ts0cos(2 fct+ i)cos(2 fct)dt+ Ts0n(t)cos(2 fct)dt=A2cos( i)+n1( ) :Z2=A Ts0cos(2 fct+ i)sin(2 fct)dt+ Ts0n(t)sin(2 fct)dt=A2sin( i)+n2( )Inthenoiselesscase,thereceivermakesuseo ftheorderedpair(Z1,Z2)=(A2cos i,A2sin i) ,letussupposethat i=90 = (Z1,Z2)as(A2cos( 2),A2sin( 2))=(0,A2).}

9 Thusthereceiverdecidesthatthecarrierphas eis (A2,0),( A2,0)and(0, A2).Thesefourpossibilitiescorrespondtoth efourphases 2,0, and3 , , , ,thereceiverwillmultiplythereceivedsigna lwithlocallygeneratedcarriersofallMfrequ encies, ,thereceivermultipliesthereceivedsignalr (t)byalocallygeneratedcosine, ( ) ,thecontinuoustimesignalr(t) (t)fori=1,2,3, , ( ).WewillseethatinthecaseofASK,N=1,inthec aseofPSKandQAM,N=2,andinthecaseofFSK,N= ,PSKandQAM,thesignalconstellationisthesa measthephasordiagramofthesignals(ignorin gthe2 fct). , (t),wecanthenwriteinvectornotation:Z=si+ n( ) , (t)wastransmitted, m= , (t),i=1,2,3, ,MthatlastforadurationTssecondseach,itis possibletoestablishthattheycanberepresen tedaselementsofafinitevectorspace(seeCha pter6)spannedbyasetoforthonormalbasisfun ctions 1(t), 2(t), , N(t)whereN , ,weassumethatthe706 ThePhysicalLayerofCommunicationsSystems 2(t) 1(t) 3(t) T3s1s2s3s4 T3 ,wecaneasilyexpressthesignalsasvectorsas follows:s1=( T3,0,0)s2=( T3, T3,0)( )s3=(0, T3, T3)s4=( T3, T3, T3)( )Thefoursignalsareplottedinthevectorsubs pacespannedby 1(t), 2(t)and 3(t) (t)eachofdurationTsseconds,itispossiblet odecomposethesesignalsintoanN( M)dimensionalvectorspacespannedbyNbasisf unctions j(t) :si(t)=N j=1sij j(t)ORsi=(si1,si2, ,siN)( )Wecancomputethecomponentsofsi(t),namely sijusingthefollowingexpression.

10 Sij= Ts0si(t) j(t)dt( )MODULATION707 Decision Boundary k(t) l(t)S2dij/2nsisjZ i(t)S1 j(t) (t)with j(t) (n1,n2, ,nN).Thecomponentsofnareindependentandid enticallydistributed( (t)wastransmitted,thereceivedsignalr(t)= si(t)+n(t).Wecanwriter(t)asavectorZ=(Z1, Z2, ,ZN)where:Zj= Ts0r(t) j(t)dt= Ts0si(t) j(t)dt+ Ts0n(t) j(t)dt=sij+nj( )Invectornotation,Z=si+n( ) decisionboundary , , , , ,ifthenoisevectorhasacomponentthatislarg erthandij2inthecorrectdirectionalongthel inejoiningsiandsj, , , ,itispossibletoshowthattheprobabilitytha tthereceiverpickss1giventhats2wastransmi ttedorviceversaisgivenby:Pe=12erfc d24N0 ( ) ( )and( ),wecanseethatthesignalsdependonlyoncos( 2 fct).Itcanbeshownthat: 1(t)= 2 Tscos(2 fct),( ) 1(t) (t) ,Eb=A22Ts A= 2 EbTs( )WecanrewritethesignalsforBPSKas:si(t)= Acos((2 fct),0 t Tsorsi(t)= 2 EbTscos(2 fct),0 t Ts( )Clearly,s1(t)= Eb 1(t)ands2(t)= Eb 1(t).Invectornotation,s1= Ebands2= (a).))


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