wireless communications - chapter 5 - mobile radio propagation(05-10)

wireless communications - chapter 5 - mobile radio propagation(05-10)

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时间:2019-03-07

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1、Chapter5.MobileRadioPropagationSmall-ScalefadingandmultiPath¢Small-ScaleMultipath°ImpulseResponseModelofaMultipathCh.°Small-ScaleMultipathMeasurements°ParametersofMobileMultipathChannel°TypesofSmall-ScaleFading°RayleighandRiceanDistributions°StatisticalModelsforMultipat

2、hFadingCh.5.1Small-ScaleMultipathPropagation°Small-scalefading,orsimplyfading,isusedtodescribetherapidfluctuationsoftheamplitudes,phases,ormultipathdelaysofaradiosignaloverashortperiodoftimeortraveldistance,sothatlarge-scalepathlosseffectsmaybeignored.°Fadingiscausedbyi

3、nterferencebetweentwoormoreversionsofthetransmittedsignalwhicharriveatthereceiveratslightlydifferenttimes.°Multipathintheradiochannelcreatessmall-scalefadingeffects.°Mostimportanteffects:(1)Rapidchangesinsignalstrengthoverasmalltraveldistanceortimeinterval;(2)Randomfreq

4、uencymodulationduetovaryingDopplershiftsondifferentmultipathsignals;(3)Timedispersion(echoes)causedbymultipathpropagationdelays.¢FactorsInfluencingSmall-ScaleFading:(1)Multipathpropagation-signalsmearingduetoISI.(2)Speedofthemobile-randomfrequencymodulationduetodifferen

5、tDopplershiftsoneachofthemultipathcomponents.(3)Speedofsurroundingobjects-timevaryingDopplershiftonmultipathcomponents.(4)Thetransmissionbandwidthofthesignal-transmittedradiosignalbandwidthisgreaterthanthe“bandwidth”ofthemultipathchannel,thereceivedsignalwillbedistorted

6、.°DopplerShift22π∆lvπ∆t由路程差造成的接收信号相位变化为:∆=ϕ=cosθλλ1∆ϕv频率变化,即多普勒频移ff为:=⋅=⋅cosθdd2πλ∆tS∆lθθXdYv5.2ImpulseResponseModelofaMultipathCh..°Thesmall-scalevariationscandirectlyrelatedtotheimpulseresponseofmobilech.;°Theimpulseresponseisawidebandchannelcharacterizationandcontain

7、sallinformationnecessarytosimulateoranalyzeanytypeofradiotransmissionthroughthechannel;°Amobilechannelmaybemodeledasalinearfilterwithatimevaryingimpulseresponse.°ImpulseResponseModelofaMultipathChannelxt()hthtejωctyt()ct()1(,)rt()(,ττ)=Re{b(,)}2htbτ带通信道的冲击响应模型基带的等效信道冲击响

8、应模型1y(t)=⊗xt()h(t)r(t)=ct()⊗h(t)b2xt()==Re{}ct()exp()j2ππfccty(t)Re{}r(t)exp()j2ftL−1htbl(,τα)=+∑(t,τ)exp⎡⎤⎣⎦j

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