现代无线通信原理全册配套完整精品课件.ppt
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1、About the Course Principles of Modern Wireless Communications 现代无线通信原理全册配套现代无线通信原理全册配套 完整精品课件完整精品课件 About the Course Principles of Modern Wireless Communications Chapter 1 Introduction to Wireless Communications About the Course Principles of Modern Wireless Communications 2 Contents: About the Cour
2、se History Services Requirements Technical Challenges About the Course Principles of Modern Wireless Communications About the Course About the Course Principles of Modern Wireless Communications 4 Objectives Study principles unique to wireless commun. Wireless channel modeling Digital modulation OFD
3、M )( )( ) c n jft nn n hta t et 2( )2 ( ) ( )( ) ( ) Re( )( ) c nc l nn n jftjf t nln n r t r ta t s tt a t es tte Technical Challenges Principles of Modern Wireless Communications Small-Scale Fading (Cont.) 59 Given sl(t) = 1, we have the received signal expressed as 2( )( ) ( )( )( ) c nn jftjt ln
4、n nn r ta t ea t e Notes: a) The received signal consists of the sum of a number of time-variant phasors. b) The phase n(t) = 2fcn(t) will change by 2 whenever n changes by 1/ fc. c) The signal can be modeled as a random process, i.e. a complex-valued Gaussian random process according to the central
5、 limit theorem. d) The signal fading, i.e. amplitude variations, may be destructive or constructive, which is primarily a result of the time variations in the n(t). Technical Challenges Principles of Modern Wireless Communications Power Delay Profile 60 Assume that h(;t) is wide-sense stationary, th
6、e autocorrelation of h(;t) is * 1212 112 1 ( ,;)( ; ) (;) 2 ( ;) () h h tE ht htt t Note the scattering at two different delays are uncorrelated. Let t = 0, the resulting autocorrelation function is h(; 0) h(), i.e. the average power output of the channel as a function of the time delay . h() is cal
7、led power delay profile. Generally speaking, h(; t) gives average power output of the channel as a function of and the difference t in observation time. Hence, the PDP may be time varying. Technical Challenges Principles of Modern Wireless Communications Time-varying impulse response 61 Technical Ch
8、allenges Principles of Modern Wireless Communications Measured impulse responses 62 Technical Challenges Principles of Modern Wireless Communications Frequency Selectivity of Channel 63 The FT of h(;t) with respect to (w.r.t.) yields the time-variant transfer function H(f;t) as 2 ( ; )( ; ) jf H f t
9、ht ed Since H(f;t) has the same statistics as h(;t), we have the autocorrelation function * 1212 1 (,;)(; )(;) 2 (;) H H fftE Hf t H f tt ft resulting from the uncorrelation of different rays. Technical Challenges Principles of Modern Wireless Communications Frequency Selectivity of Channel (Cont.)
10、64 For t = 0, H(f; 0) H(f), which can be derived from the FT of h() 2 ()( ) jf Hh fed which provides us with a measure of the frequency coherence of the channel. The coherence bandwidth of the channel is measured as max 1 c B where max denotes the multipath delay. If the bandwidth of the transmitted
11、 signal Bs Bc, the channel is frequency-selective. Otherwise, the channel is frequency-nonselective, i.e. flat fading. Technical Challenges Principles of Modern Wireless Communications Time Selectivity of Channel 65 The FT of H(f; t) w.r.t. t gives the function as 2 (; )(;)() jt HH Sfft edt If f = 0
12、, SH(f; ) SH(), which is the Doppler power spectrum given by 2 ( )(0;)() jt HH St edt The coherence time of the channel is related to the Doppler spread Fd as 1 c d T F Technical Challenges Principles of Modern Wireless Communications Time-Varying CFR 66 Technical Challenges Principles of Modern Wir
13、eless Communications Scattering Function Understand the variables (; f) as well as (t; ) The FT between H(f; t) and h(; t) The FT between H(f; t) and SH(f; ) A closed-loop relationship is obtained by defining a new function, i.e. the scattering function of the channel. 67 22 2 2 ( ; )(;)() () ( ;)()
14、 (; )() jtjf H jt h jf H Sft eedt df t edt Sfedf Technical Challenges Principles of Modern Wireless Communications Two Independent Fading Issues 68 Technical Challenges Principles of Modern Wireless Communications Time Dispersion (flat) 69 Technical Challenges Principles of Modern Wireless Communica
15、tions Time Dispersion (selec.) 70 Technical Challenges Principles of Modern Wireless Communications Doppler Shift Geomerty 71 From X Y, the phase difference 22 cos cc lv t The frequency variation is the Doppler shift 1 coscos 2 c d c vvf f tc Technical Challenges Principles of Modern Wireless Commun
16、ications Channel Statistics 72 For each resolvable path, the channel gain is considered as a sum of M components, of which the amplitude and the phase are random processes. 1 11 (cossin n M jt n n MM nnnn nn IQ u tut e uttjutt utjut If M 8, we consider R.V. , then u(t) follows Rayleigh distribution.
17、 2 ,(0,) IQ ututN 2 2 2 2 , 0 u u p ueu Technical Challenges Principles of Modern Wireless Communications Channel Statistics 73 In the presence of a LOS ray or a specularly reflected path, we have 00 1 2 2 (2) 0 ( ) c jff mmjm t e tt () IIQQ r tu tm t utmtj utmt Then, the envelope is Ricean distribu
18、tion. 22 0 2 0 2 2 0 2 r () r p r reI Technical Challenges Principles of Modern Wireless Communications Channel Statistics 74 RayleighRicean Technical Challenges Principles of Modern Wireless Communications Channel Statistics 75 2 00 ()(2) uum RtJft The correlation function of channel-response envel
19、ope 2 0 2 ( ),| 1() um m m Sfff f f f Then the Doppler power spectrum Other kinds of Doppler spectrum may be applied, like Gaussian spectrum in the COST207 TU channel model. Technical Challenges Principles of Modern Wireless Communications Channel Statistics 76 -100-80-60-40-20020406080100 0 0.01 0.
20、02 0.03 0.04 0.05 0.06 0.07 0.08 f/Hz S ii(f) 00.0050.010.0150.020.0250.030.0350.040.0450.05 -0.5 0 0.5 1 /s R ii() Auto-correlation functionDoppler spectrum Technical Challenges Principles of Modern Wireless Communications Modeling Wireless Channels Technical Challenges Principles of Modern Wireles
21、s Communications About Path Delay Propagation delay 2) Zero-pole filter shapes the Doppler power spectrum. Technical Challenges Principles of Modern Wireless Communications II. Frequency-Domain Shaping 86 Technical Challenges Principles of Modern Wireless Communications II. Frequency-Domain Shaping
22、High-efficiency IFFTs make fast fading simulator. Increasing spectral resolution requires large-size IFFT. Singular spectrum at fm necessitates high- resolution lines. Block-wise processing needs large-size storage. 87 Technical Challenges Principles of Modern Wireless Communications III. Method of
23、Sum-Of-Sinusoids (SOS) 88 Clarke Model: 1 2 ( )exp cos() N mnn n g tjt N Note the angle of arrival (AoA) n and the initial phase n are independent RVs, and n, n U-, ) . Jakes Model: 1) Simplify the AoA: n = 2n/N 2) Introduce phase relation between rays M = (N-2)/4 sinusoids Technical Challenges Prin
24、ciples of Modern Wireless Communications 89 Technical Challenges Principles of Modern Wireless Communications III. Method of Sum-Of-Sinusoids (SOS) 90 -100-50050100 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 Technical Challenges Principles of Modern Wireless Communications III. Method of Sum-Of-Sinusoids (SO
25、S) 91 00.511.522.53 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 Amplitude Simulator of Jake Model r/ P(r) 2=0.5 theoretical N=8 N=16 N=34 Technical Challenges Principles of Modern Wireless Communications III. Method of Sum-Of-Sinusoids (SOS) 92 00.050.10.150.2 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 AutoC
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