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https://github.com/BreizhHardware/cours-ISEN-MD.git
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173 lines
4.5 KiB
Matlab
173 lines
4.5 KiB
Matlab
%% Experiment 2 : Raised cosine with jamming and ambient noise
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% - Generate raised cosine h(t) on [-10T, 10T], T = 2 ms, beta = 0.5
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% - Sampling period Ts = 0.13*T
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% - Add narrowband jamming at 800 Hz and white noise
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% - Design IIR notch filter (order 15 then 5) to remove the jamming tone
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% - Use subplot to show time-domain signal and magnitude spectrum.
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clc;
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clear;
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close all;
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%% 1) Parameters and time vector
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T = 2e-3; % Symbol period (s)
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beta = 0.5; % Roll-off factor
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Ts = 0.13 * T; % Sampling period (s)
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Fs = 1 / Ts; % Sampling frequency (Hz)
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t = -10*T : Ts : 10*T; % Time vector
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N = length(t);
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% Frequency axis for spectra (centered)
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f_axis = (-N/2 : N/2-1) * (Fs / N); % Hz
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%% 2) Raised cosine pulse h(t)
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h = arrayfun(@(tt) raisedCosineSample(tt, T, beta), t);
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% Time-domain h(t) and magnitude spectrum
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H = fft(h);
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magH = abs(fftshift(H)); % magnitude, zero frequency at center
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figure('Name','Experiment 2 - h(t) and |H(f)|');
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subplot(2,1,1);
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plot(t*1e3, h, 'g');
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xlabel('Time (ms)');
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ylabel('h(t)');
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title('Raised cosine pulse h(t), \beta = 0.5');
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grid on;
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subplot(2,1,2);
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plot(f_axis, magH, 'g');
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xlabel('Frequency (Hz)');
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ylabel('|H(f)|');
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title('Magnitude spectrum |H(f)| of raised cosine');
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grid on;
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%% 3) Generate jamming and ambient noise, build z(t)
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fJam = 800; % Jamming frequency (Hz)
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x = 0.2 * cos(2*pi*fJam*t); % narrowband jamming (adjust amplitude if needed)
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n = 0.02 * randn(size(t)); % ambient white noise (low level)
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z = h + x + n; % corrupted signal
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% Time-domain and magnitude spectrum of z(t)
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Z = fft(z);
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magZ = abs(fftshift(Z));
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figure('Name','Experiment 2 - z(t) and |Z(f)|');
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subplot(2,1,1);
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plot(t*1e3, z, 'g');
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xlabel('Time (ms)');
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ylabel('z(t)');
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title('Noisy signal z(t) = h(t) + jamming + white noise');
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grid on;
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subplot(2,1,2);
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plot(f_axis, magZ, 'g');
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xlabel('Frequency (Hz)');
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ylabel('|Z(f)|');
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title('Magnitude spectrum |Z(f)| with jamming at 800 Hz');
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grid on;
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%% 4) Design 15th-order notch (bandstop) filter at 800 Hz (no butter)
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% We build an IIR notch with zeros at exp(±j*w0) and poles at r*exp(±j*w0),
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% then cascade enough sections to reach an effective order ≈ 15.
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w0 = 2*pi*fJam/Fs; % digital radian frequency
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r = 0.98; % pole radius (controls notch width)
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% One second-order notch section:
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b_sec = [1, -2*cos(w0), 1]; % zeros at e^{±jw0}
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a_sec = [1, -2*r*cos(w0), r^2]; % poles at r*e^{±jw0}
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% Approximate 15th-order by cascading 8 sections (~16th order)
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sections = 8; % adjust to get desired attenuation
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b15 = 1;
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a15 = 1;
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for k = 1:sections
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b15 = conv(b15, b_sec);
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a15 = conv(a15, a_sec);
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end
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% Filter output zz(t) and its spectrum
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zz15 = filter(b15, a15, z);
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ZZ15 = fft(zz15);
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magZZ15 = abs(fftshift(ZZ15));
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figure('Name','Experiment 2 - Order ~15 notch filter');
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subplot(2,1,1);
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plot(t*1e3, zz15, 'g');
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xlabel('Time (ms)');
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ylabel('zz_{15}(t)');
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title('Filtered signal (notch order ≈ 15)');
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grid on;
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subplot(2,1,2);
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plot(f_axis, magZZ15, 'g');
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xlabel('Frequency (Hz)');
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ylabel('|ZZ_{15}(f)|');
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title('Magnitude spectrum after order ≈ 15 notch filter');
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grid on;
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%% 5) Modify filter order to ~5 and update plot
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% Fewer cascaded sections (e.g. 3 -> ~6th order)
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sections2 = 3;
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b5 = 1;
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a5 = 1;
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for k = 1:sections2
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b5 = conv(b5, b_sec);
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a5 = conv(a5, a_sec);
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end
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zz5 = filter(b5, a5, z);
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ZZ5 = fft(zz5);
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magZZ5 = abs(fftshift(ZZ5));
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figure('Name','Experiment 2 - Order ~5 notch filter');
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subplot(2,1,1);
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plot(t*1e3, zz5, 'g');
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xlabel('Time (ms)');
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ylabel('zz_{5}(t)');
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title('Filtered signal (notch order ≈ 5)');
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grid on;
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subplot(2,1,2);
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plot(f_axis, magZZ5, 'g');
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xlabel('Frequency (Hz)');
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ylabel('|ZZ_{5}(f)|');
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title('Magnitude spectrum after order ≈ 5 notch filter');
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grid on;
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%% ===== Local function: one sample of raised cosine pulse =====
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function h = raisedCosineSample(t, T, beta)
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% Raised cosine pulse sample at time t (scalar).
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% h(t) = sinc(t/T) * cos(pi*beta*t/T) / (1 - (4*beta^2*t^2)/T^2)
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% with sinc(x) = sin(pi*x)/(pi*x).
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x = t / T;
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% Manual sinc(x)
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if abs(x) < 1e-12
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sx = 1; % limit at x -> 0
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else
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sx = sin(pi*x) / (pi*x);
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end
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% Handle critical points of the raised cosine denominator
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if abs(t) < 1e-12
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h = 1;
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elseif beta ~= 0 && abs(abs(t) - T/(2*beta)) < 1e-12
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h = (beta/pi) * sin(pi/(2*beta)); % limit at t = ±T/(2*beta)
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else
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h = sx * cos(pi*beta*x) / (1 - (4*beta^2*x^2));
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end
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end
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