Напиши подробное решение номера 1, на английском, ...

बनाया गया: 1 दिसंबर 2025

का उपयोग करके उत्तर दिया गया GPT-5.1 Thinking द्वारा Chat01

प्रश्न

HW3_2025.pdf

Напиши подробное решение номера 1, на английском, код на матлабе.

विचार

Presenting filter design and poles calculation

The Chebyshev prototype filter has poles defined by the standard formulas for σ_k and ω_k. While we could compute poles directly, it seems unnecessary for this case. Instead, I’ll focus on showing the general method and mention how to use MATLAB functions like cheb1ord/cheby1 for automatic computation. The user also asked for code and the analog impulse response using impulse().

Designing the Chebyshev filter and approximating results

For the task, I'll outline the steps for designing a Chebyshev filter using given analog specs with MATLAB’s cheb1ord and cheby1. While I can't run MATLAB, I can show code that computes the order and cutoff frequency. I might approximate results using Python formulas or mpmath if needed, but exact polynomial computations aren't necessary for the solution. Showing the key numerical values should suffice.

Designing and converting the Chebyshev filter

I'll start by designing the analog lowpass Chebyshev filter with MATLAB's cheby1 function. Then, I'll convert it to digital using impulse invariance with impinvar. For impulse responses, I'll use MATLAB's impulse for the analog case and impz for the digital case. Finally, I'll plot the responses and compute the frequency response with freqs and freqz.

Plotting analog and digital frequency responses

For the analog case, I'll define a frequency range and use MATLAB's freqs function for the response. For the digital case, I'll use freqz. Then, I'll plot the magnitude in dB. I'll also overlay analog and digital magnitude responses, addressing how aliasing can affect the mapped frequencies when using impulse invariance.

Thought for 2m 56s

उत्तर

Problem 1 is: design a Chebyshev analog low-pass filter with given specs and then obtain the digital filter via impulse invariance, then plot impulse and magnitude responses for both. (HW3_2025.pdf)

Below is a detailed solution in English plus ready-to-run MATLAB code at the end.


1. Given specifications

  • Passband edge frequency (analog):
    fp=18MHzf_p = 18\,\text{MHz}
  • Stopband edge frequency (analog):
    fs=20MHzf_s = 20\,\text{MHz}
  • Passband ripple:
    Ap=0.3dBA_p = 0.3\,\text{dB}
  • Stopband attenuation:
    As=60dBA_s = 60\,\text{dB}
  • Sampling frequency for the digital filter:
    Fs=50MHzF_s = 50\,\text{MHz}
    so sampling period
    T=1Fs=20nsT = \dfrac{1}{F_s} = 20\,\text{ns}

We first design the analog Chebyshev Type I low-pass filter, then convert it to a digital IIR filter by impulse invariance.


2. Convert specs to angular frequencies

Use

Ω=2πf\Omega = 2\pi f
  • Passband edge (rad/s): Ωp=2πfp=2π18×106\Omega_p = 2\pi f_p = 2\pi \cdot 18 \times 10^6
  • Stopband edge (rad/s): Ωs=2πfs=2π20×106\Omega_s = 2\pi f_s = 2\pi \cdot 20 \times 10^6

In MATLAB we’ll store these as:

matlab
Fp = 18e6; % Hz Fs1 = 20e6; % Hz (stopband edge) Wp = 2*pi*Fp; % rad/s Ws = 2*pi*Fs1; % rad/s

Note: the ratio of stopband to passband edge (in rad/s or Hz) is the same:

ΩsΩp=fsfp=20181.1111\frac{\Omega_s}{\Omega_p} = \frac{f_s}{f_p} = \frac{20}{18} \approx 1.1111

3. Chebyshev Type I filter parameters

A Chebyshev Type I lowpass filter has magnitude squared:

Ha(jΩ)2=11+ε2TN2(ΩΩc)|H_a(j\Omega)|^2 = \frac{1}{1 + \varepsilon^2\,T_N^2\left(\frac{\Omega}{\Omega_c}\right)}

Where:

  • NN is filter order,
  • TN()T_N(\cdot) is the Chebyshev polynomial of degree NN,
  • ε\varepsilon is the ripple factor,
  • Ωc\Omega_c is the cutoff parameter.

3.1 Ripple factor ε\varepsilon

Passband ripple in dB is related to ε\varepsilon via:

Ap=10log10(1+ε2)ε=10Ap/101A_p = 10\log_{10}\left(1+\varepsilon^2\right) \quad\Rightarrow\quad \varepsilon = \sqrt{10^{A_p/10} - 1}

For Ap=0.3dBA_p = 0.3\,\text{dB}:

ε=100.3/1010.2674\varepsilon = \sqrt{10^{0.3/10} - 1} \approx 0.2674

(We’ll let MATLAB compute this numerically for us.)

3.2 Stopband condition and order NN

The stopband attenuation is:

As=10log10(1+ε2TN2(ΩsΩc))A_s = 10\log_{10}\left(1+\varepsilon^2 T_N^2\left(\frac{\Omega_s}{\Omega_c}\right)\right)

For a lowpass with passband edge at Ωp\Omega_p, we usually normalize such that Ωp\Omega_p is at the passband edge and we compare Ωs/Ωp\Omega_s/\Omega_p.

The formula for the minimum Chebyshev order is:

Ncosh1(10As/10110Ap/101)cosh1(ΩsΩp)N \ge \frac{\cosh^{-1}\left(\sqrt{\frac{10^{A_s/10}-1}{10^{A_p/10}-1}}\right)} {\cosh^{-1}\left(\frac{\Omega_s}{\Omega_p}\right)}

Let

ε=10Ap/101,A=10As/101,k=ΩsΩp=fsfp.\begin{aligned} \varepsilon &= \sqrt{10^{A_p/10} - 1},\\ A &= \sqrt{10^{A_s/10} - 1}, \\ k &= \frac{\Omega_s}{\Omega_p} = \frac{f_s}{f_p}. \end{aligned}

Then

Ncosh1(A/ε)cosh1(k).N \ge \frac{\cosh^{-1}(A/\varepsilon)}{\cosh^{-1}(k)}.

Numerically (approximate):

  • ε0.2674\varepsilon \approx 0.2674
  • A1000A \approx 1000
  • k=20/181.1111k = 20/18 \approx 1.1111
  • N19.09N=20N \approx 19.09 \Rightarrow N = 20 (must be an integer, so we round up).

So the analog Chebyshev filter will be order 20.

In practice, MATLAB can calculate NN and the cutoff frequency WcW_c for us with cheb1ord.


4. Analog Chebyshev filter design (in MATLAB)

We now design the analog lowpass with these specs:

matlab
Rp = 0.3; % passband ripple in dB Rs = 60; % stopband attenuation in dB [N, Wc] = cheb1ord(Wp, Ws, Rp, Rs, 's'); % analog (s-plane) design % N = filter order (should come out as 20) % Wc = cutoff rad/s (Chebyshev cutoff)

Then use cheby1 to get numerator and denominator of Ha(s)H_a(s):

matlab
[ba, aa] = cheby1(N, Rp, Wc, 'low', 's'); % analog Chebyshev Type I, lowpass

So the analog transfer function is:

Ha(s)=Ba(s)Aa(s)=b0sN+b1sN1++bNsN+a1sN1++aNH_a(s) = \frac{B_a(s)}{A_a(s)} = \frac{b_0 s^{N} + b_1 s^{N-1} + \cdots + b_N} {s^{N} + a_1 s^{N-1} + \cdots + a_N}

where ba and aa store the coefficients of the numerator and denominator.


5. Impulse invariance method

5.1 Concept

Let:

  • ha(t)h_a(t) be the impulse response of the analog filter Ha(s)H_a(s).
  • Sampling period T=1/FsT = 1/F_s.

Impulse invariance defines the digital impulse response as:

h[n]=Tha(nT),n=0,1,2,h[n] = T \, h_a(nT), \quad n = 0,1,2,\ldots

This ensures that each analog pole sks_k maps to a digital pole

zk=eskT.z_k = e^{s_k T}.

The corresponding digital transfer function can be found by a partial fraction expansion or, more conveniently, with MATLAB’s impinvar function:

matlab
[bz, az] = impinvar(ba, aa, Fs);

This directly gives you the discrete-time filter:

H(z)=B(z)A(z)=b0+b1z1++bMzM1+a1z1++aMzMH(z) = \frac{B(z)}{A(z)} = \frac{b_0 + b_1 z^{-1} + \cdots + b_M z^{-M}} {1 + a_1 z^{-1} + \cdots + a_M z^{-M}}

Note: Impulse invariance preserves the shape of the impulse response (sampled) but causes aliasing in the frequency domain; here we assume that the analog filter is sufficiently attenuated above Nyquist (25 MHz) so that aliasing is not critical.


6. Impulse responses (analog and digital)

6.1 Analog impulse response

We can obtain ha(t)h_a(t) for a selected time interval using Control System Toolbox:

matlab
t_max = 10/Fp; % e.g. several periods of passband edge t = linspace(0, t_max, 2000); % time vector Ha_sys = tf(ba, aa); % continuous-time transfer function ha = impulse(Ha_sys, t); % analog impulse response

6.2 Digital impulse response

For the digital filter we use impz:

matlab
N_imp = 200; % number of samples to show [hd, n] = impz(bz, az, N_imp); % digital impulse response

We then plot and compare:

  • Analog: ha(t)h_a(t) vs. tt
  • Digital: h[n]h[n] vs. nn

7. Magnitude responses (analog and digital)

7.1 Analog magnitude response

Use freqs for continuous-time filters. To compare with the digital case we’ll plot Analog frequency in Hz rather than rad/s:

matlab
w_max = 2*pi*25e6; % up to 25 MHz (Nyquist of digital system) w = linspace(0, w_max, 4096); % rad/s Ha_w = freqs(ba, aa, w); % analog frequency response fa = w / (2*pi); % Hz MagHa_dB = 20*log10(abs(Ha_w)); % magnitude in dB

7.2 Digital magnitude response

Use freqz with sampling frequency Fs so the frequency axis is in Hz:

matlab
[Hd_w, fd] = freqz(bz, az, 4096, Fs); % fd in Hz MagHd_dB = 20*log10(abs(Hd_w));

We can then plot both on the same figure (or separate figures) to compare magnitude responses as functions of frequency up to 25 MHz.


8. Complete MATLAB code

Below is a single self-contained MATLAB script that:

  1. Designs the analog Chebyshev filter,
  2. Converts it to digital using impulse invariance,
  3. Plots impulse responses of analog and digital filters,
  4. Plots magnitude responses of analog and digital filters.
matlab
%% Problem 1: Chebyshev LPF + Impulse Invariance clear; clc; close all; %% Given specifications Fp = 18e6; % passband edge frequency (Hz) Fs1 = 20e6; % stopband edge frequency (Hz) Rp = 0.3; % passband ripple (dB) Rs = 60; % stopband attenuation (dB) Fs = 50e6; % sampling frequency for digital filter (Hz) T = 1/Fs; % sampling period (s) % Analog radian frequencies Wp = 2*pi*Fp; % passband edge (rad/s) Ws = 2*pi*Fs1; % stopband edge (rad/s) %% 1) Analog Chebyshev Type I design % Determine filter order and cutoff [N, Wc] = cheb1ord(Wp, Ws, Rp, Rs, 's'); fprintf('Analog Chebyshev filter order N = %d\n', N); % Design analog Chebyshev Type I lowpass (s-domain) [ba, aa] = cheby1(N, Rp, Wc, 'low', 's'); % Analog transfer function H_a(s) Ha_sys = tf(ba, aa); % requires Control System Toolbox %% 2) Impulse invariance: analog -> digital % Obtain digital IIR filter using impulse invariance [bz, az] = impinvar(ba, aa, Fs); %% 3) Impulse responses % --- Analog impulse response --- t_max = 10/Fp; % choose a suitable time span t = linspace(0, t_max, 2000); % time vector ha = impulse(Ha_sys, t); % --- Digital impulse response --- N_imp = 200; % number of samples for impulse response [hd, n] = impz(bz, az, N_imp); % digital impulse response % Plot impulse responses figure; subplot(2,1,1); plot(t, ha, 'LineWidth', 1.2); grid on; xlabel('t (s)'); ylabel('h_a(t)'); title('Analog Impulse Response'); subplot(2,1,2); stem(n, hd, 'filled'); grid on; xlabel('n'); ylabel('h[n]'); title('Digital Impulse Response (Impulse Invariance)'); %% 4) Magnitude responses % --- Analog magnitude response --- w_max = 2*pi*25e6; % plot up to 25 MHz (Nyquist of digital system) w = linspace(0, w_max, 4096); % rad/s Ha_w = freqs(ba, aa, w); % analog freq response fa = w / (2*pi); % frequency axis in Hz MagHa_dB = 20*log10(abs(Ha_w)); % --- Digital magnitude response --- [Hd_w, fd] = freqz(bz, az, 4096, Fs); % fd in Hz MagHd_dB = 20*log10(abs(Hd_w)); % Plot magnitude responses figure; subplot(2,1,1); plot(fa/1e6, MagHa_dB, 'LineWidth', 1.2); grid on; xlabel('Frequency (MHz)'); ylabel('|H_a(j\Omega)| (dB)'); title('Analog Chebyshev LPF Magnitude Response'); xlim([0 25]); % show 0–25 MHz subplot(2,1,2); plot(fd/1e6, MagHd_dB, 'LineWidth', 1.2); grid on; xlabel('Frequency (MHz)'); ylabel('|H_d(e^{j\omega})| (dB)'); title('Digital IIR (Impulse Invariance) Magnitude Response'); xlim([0 25]); % 0–25 MHz (Nyquist)

If you’d like, I can also add comments showing how to extract and write down the difference equation of the resulting digital filter H(z)H(z) from the bz and az coefficients.

प्रश्न

Warning: The output is not correct/robust. Coeffs of B(s)/A(s) are real, but B(z)/A(z) has complex
coeffs. Probable cause is rooting of high-order repeated poles in A(s).
B(z) and A(z) have been forced to be real using real(A(z)) and real(B(z)).

In impinvar (line 130)
In problem1 (line 30)

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