Preview only show first 10 pages with watermark. For full document please download

Modelling Multipath Signals Direct Signal, Angle Of Arrival

   EMBED


Share

Transcript

Lecture ( 4 Mar. 2015) 4/25/2015 Modelling Multipath Signals Direct Signal, Angle of Arrival and Doppler Shift 1 Lecture ( 4 Mar. 2015) 4/25/2015 Direct Signal, Angle of Arrival and Doppler Shift / / / / / / Direct Signal, Angle of Arrival and Doppler Shift 2 Lecture ( 4 Mar. 2015) 4/25/2015 Direct Signal, Angle of Arrival and Doppler Shift Direct Signal, Angle of Arrival and Doppler Shift 3 Lecture ( 4 Mar. 2015) 4/25/2015 Direct Signal, Angle of Arrival and Doppler Shift Direct Signal, Angle of Arrival and Doppler Shift 4 Lecture ( 4 Mar. 2015) 4/25/2015 Direct Signal, Angle of Arrival and Doppler Shift Matlab Code [1/4] clear all; close all; clc; % basic inputs ============================= fc=2e9; % Hz Carrier frequency F=16; % sampling rate: fraction of wave length V=10; % m/s MS1 speed NFFT=128; % Number of points in FFT Nsamples=100; % Number of samples % geometry inputs =========================== dBS=1000; % distance of BS to origin alpha = 180; % degree. Angle of BS-MS with MS route % inidirect gemeotric parameters ================ BSx=dBS*cosd(alpha); % loc of BS x-coord BSy=dBS*sind(alpha); % loc of BS y-coord 5 Lecture ( 4 Mar. 2015) 4/25/2015 Matlab Code [2/4] % indirect parameters =========================== c=3e8; lambdac=c/fc; % m wavelength Dx=lambdac/F; % m sampling spacing ts=Dx/V; % s time sampling interval fs=1/ts; % Hz sampling frequency kc=2*pi/lambdac; % propagation constant timeaxis=ts.*[0:Nsamples]; disaxis=Dx.*[0:Nsamples]; % s elapsed time axis % n traveled distance axis MSx=V.*timeaxis; % MS route sampling points % radio path length============================== distBSMS=sqrt((BSx-MSx).^2+(BSy).^2); Matlab Code [3/4] % complex envelope: amplitude and phase =============== r=1*exp(-j*kc.*distBSMS); % complex envelope spectrum ====================== spectrumr=fftshift((abs(fft(r,NFFT))).^2); freqaxis=[0:NFFT-1]*fs/NFFT-fs/2; 6 Lecture ( 4 Mar. 2015) 4/25/2015 Matlab Code [4/4] % Plots ===================================== figure,plot(timeaxis,abs(r)) xlabel('Time (s)') ; ylabel('Magnitude of complex envelope'); figure,plot(disaxis,unwrap(angle(r))) xlabel('Traveled distance (m)'); ylabel('Absolute phase of complex envelope (rad)'); figure,plot(disaxis,angle(r)) xlabel('Traveled distance (m)'); ylabel('Modulo-\pi phase of complex envelope (rad)') figure,plot(freqaxis,10*log10(spectrumr)-max(10*log10(spectrumr))) xlabel('Doppler shift (Hz)') ylabel('Normalized frquency response (dB)') Direct and Reflected Signals D= DR= 7 Lecture ( 4 Mar. 2015) 4/25/2015 Direct and Reflected Signals DR= D= Direct and Reflected Signals D= DR= 8 Lecture ( 4 Mar. 2015) 4/25/2015 Direct and Reflected Signals D= DR= Dropping fixed phases, Direct and Reflected Signals 9 Lecture ( 4 Mar. 2015) 4/25/2015 Direct and Reflected Signals Two Scatterers No LoS signal 10 Lecture ( 4 Mar. 2015) 4/25/2015 Two Scatterers Two Scattering points 11 Lecture ( 4 Mar. 2015) 4/25/2015 Two Scattering points Multiple Scattering points 12 Lecture ( 4 Mar. 2015) 4/25/2015 Multiple Scattering points Multiple Scattering points 13 Lecture ( 4 Mar. 2015) 4/25/2015 Mobile-to-Mobile Communications Assignment 2 Question No. 1: Find a relationship for the Doppler shift frequency and complex envelopes of the received signal if the transmitted signal is an unmodulated RF signal. • mobile-to-mobile communication scenario, i.e., both ends are moving. • Initial distance between M1 and M2 is d. • Only LoS path exist (single path). • M1 is moving with a velocity v1 and M2 is moving with a velocity v2, directly towards/away-from each other. Question No. 2: Repeat question no. 1 for a the direction of MSs’ motion generalized by parameter α, i.e., • M1 is moving in a direction α1 w.r.t. LoS path with a velocity v1. • M2 is moving in a direction α2 w.r.t. LoS path .with a velocity v2. Question No. 3: Extend simulations in question no. 2 by taking multipath into account. Take fixed number of reflectors at fixed locations. 14 Lecture ( 4 Mar. 2015) 4/25/2015 The Clarke’s Model p(α) 0 α The Clarke’s Model 15 Lecture ( 4 Mar. 2015) 4/25/2015 Fading Statistics • Second order statistics • Level Crossing Rate (lcr). The average number of times the signal crosses a given threshold, R, within a given observation time, T, with either a positive or negative slope • Average Fade Duration (afd). The ratio between the total time the received signal is below a reference level, R, and the total number of fades. o These two parameters are of interest since they can help in the selection of the most suitable error protection coding scheme and interleaving algorithm. o The afd helps determine the most likely number of bits that may be lost during a fade. Second order statistics (lcr) R lcr: ; 16 Lecture ( 4 Mar. 2015) 4/25/2015 Second order statistics (afd) R afd: For Rayleigh distribution case: Second order statistics 17 Lecture ( 4 Mar. 2015) 4/25/2015 Second order statistics In order to detect about 50% of the fades (i.e., 30 dB) below the rms level, the signal must be sampled every 0.0126λ, which means a fraction, F, of the wavelength of approximately 79. Random FM • Channel gives rise to random amplitude and phase variations, together with Doppler shifts. • One further effect caused by the channel is random frequency modulation. • Random FM, which is more marked at the deep fades, can be considered as an additional noise source affecting the transmitted signal, especially if a frequency-sensitive detector is used. • The random FM caused by the channel can be calculated as, 18 Lecture ( 4 Mar. 2015) 4/25/2015 Random FM Autocorrelation of complex envelops. 19 Lecture ( 4 Mar. 2015) 4/25/2015 Directional Antenna A directional antenna is an antenna which radiates higher power in selective directions. Using Directional Antenna p(α) γ 0 α 20 Lecture ( 4 Mar. 2015) 4/25/2015 Using Directional Antenna A narrower spectrum means slower variations. Using Directional Antenna A wider spectrum means faster variations. 21 Lecture ( 4 Mar. 2015) 4/25/2015 Angle- and Time- of-Arrival Statistics (USM) AoA: Distribution of power w.r.t. physical angles of arriving multipath signals. ToA: Distribution of power w.r.t. delay of arriving multipath signals. Angle- and Time- of-Arrival Statistics (GSM). 22 Lecture ( 4 Mar. 2015) 4/25/2015 Angular Shape factors • Angular Span • Angular Spread. • Shape factor Angular Shape factors • Mean of AoA • Direction of Maximum fading. • Angular Constriction 23 Lecture ( 4 Mar. 2015) 4/25/2015 Angular Spread (Shape factor) Angular Constriction 24