Skip to main content

How Windowing Affects Your Periodogram


The windowed periodogram is a widely used technique for estimating the Power Spectral Density (PSD) of a signal. It enhances the classical periodogram by mitigating spectral leakage through the application of a windowing function. This technique is essential in signal processing for accurate frequency-domain analysis.

 

Power Spectral Density (PSD)

The PSD characterizes how the power of a signal is distributed across different frequency components. For a discrete-time signal, the PSD is defined as the Fourier Transform of the signal’s autocorrelation function:

Sx(f) = FT{Rx(Ï„)}

Here, Rx(Ï„)}is the autocorrelation function.

FT : Fourier Transform

 

Classical Periodogram

The periodogram is a non-parametric PSD estimation method based on the Discrete Fourier Transform (DFT):

Px(f) = \(\frac{1}{N}\) X(f)2

Here:

  • X(f): DFT of the signal x(n)

  • N: Signal length

However, the classical periodogram suffers from spectral leakage due to abrupt truncation of the signal.

 

Windowing to Mitigate Spectral Leakage

Spectral leakage can be minimized by applying a window function to the signal before computing the DFT. The resulting PSD estimate is called the windowed periodogram:

Pw(f) = \(\frac{1}{NW}\) Xw(f)2

Here:

  • w(n): Window function

  • W: Window normalization factor

Common Window Functions

  • Rectangular Window: Equivalent to the classical periodogram.

w[n]=1, 0≤n≤N−1

w[n]=0, otherwise

Where, N is the window length

  • Hamming Window: Reduces sidelobe amplitudes, improving frequency resolution.

w[n]=0.5(1−cos(\(\frac{\ 2\pi n}{N - 1}\ \))), 0≤n≤N−1

Where, N is the window length

  • Hanning Window: Similar to Hamming but with less sidelobe attenuation.

w[n]=0.54 – 0.46cos(\(\frac{\ 2\pi n}{N - 1}\ \)), 0≤n≤N−1

Where, N is the window length

  • Blackman Window: Offers even greater sidelobe suppression but at the cost of wider main lobes.

w[n]=0.42 – 0.5(cos(\(\frac{\ 2\pi n}{N - 1}\ \)) + 0.08(cos(\(\frac{\ 4\pi n}{N - 1}\ \)), 0≤n≤N−1

Where, N is the window length

 

Implementation Steps

  1. Segment the Signal: Divide the signal into overlapping or non-overlapping segments of length N.

  2. Apply a Window Function: Multiply each segment by a window function w(n).

  3. Compute the DFT: Calculate the DFT of the windowed segments.

  4. Average the Periodograms: For overlapping segments, average the periodograms to reduce variance.

     

Properties of the Windowed Periodogram

  • Bias: Windowing introduces bias in the PSD estimate as the window modifies the signal spectrum.

  • Variance: Averaging periodograms (Welch method) reduces variance but decreases frequency resolution.

  • Trade-Off: The choice of window affects the trade-off between spectral resolution and leakage suppression.

     

    MATLAB Code

    clc;
    clear;
    close all;

    fs = 48000;
    t = 0:1/fs:0.02;
    f_ping = 12000;

    % Base sine wave
    sine_wave = sin(2*pi*f_ping*t)';

    % Apply windows
    w_rect = ones(size(sine_wave));
    w_hann = hann(length(sine_wave));
    w_hamming = hamming(length(sine_wave));
    w_blackman = blackman(length(sine_wave));

    % Windowed signals
    s_rect = sine_wave .* w_rect;
    s_hann = sine_wave .* w_hann;
    s_hamming = sine_wave .* w_hamming;
    s_blackman = sine_wave .* w_blackman;

    % FFT
    Nfft = 4096;
    f = fs*(0:Nfft/2-1)/Nfft;

    % Function to compute and normalize spectrum
    get_norm_fft = @(sig) abs(fft(sig, Nfft))/max(abs(fft(sig, Nfft)));

    S_rect = get_norm_fft(s_rect);
    S_hann = get_norm_fft(s_hann);
    S_hamming = get_norm_fft(s_hamming);
    S_blackman = get_norm_fft(s_blackman);

    % Mainlobe power (±2 bins around peak)
    mainlobe_bins = 2;

    % Function to compute power ratio
    compute_power_ratio = @(S) ...
    deal( ...
    sum(S.^2), ... % Total power
    max(1, find(S == max(S), 1)), ... % Peak bin
    @(peak_bin) sum(S(max(1,peak_bin-mainlobe_bins):min(Nfft,peak_bin+mainlobe_bins)).^2), ...
    @(total, main) 10*log10((total-main)/main) ... % dB sidelobe/mainlobe ratio
    );

    % Calculate ratios
    [total_r, peak_r, get_main_r, get_slr_r] = compute_power_ratio(S_rect);
    main_r = get_main_r(peak_r); slr_r = get_slr_r(total_r, main_r);

    [total_h, peak_h, get_main_h, get_slr_h] = compute_power_ratio(S_hann);
    main_h = get_main_h(peak_h); slr_h = get_slr_h(total_h, main_h);

    [total_ham, peak_ham, get_main_ham, get_slr_ham] = compute_power_ratio(S_hamming);
    main_ham = get_main_ham(peak_ham); slr_ham = get_slr_ham(total_ham, main_ham);

    [total_b, peak_b, get_main_b, get_slr_b] = compute_power_ratio(S_blackman);
    main_b = get_main_b(peak_b); slr_b = get_slr_b(total_b, main_b);

    % Display Results
    fprintf('Window | Mainlobe Power | Sidelobe Power | Sidelobe/Main (dB)\n');
    fprintf('------------|----------------|----------------|--------------------\n');
    fprintf('Rectangular | %14.4f | %14.4f | %18.2f\n', main_r, total_r - main_r, slr_r);
    fprintf('Hann | %14.4f | %14.4f | %18.2f\n', main_h, total_h - main_h, slr_h);
    fprintf('Hamming | %14.4f | %14.4f | %18.2f\n', main_ham, total_ham - main_ham, slr_ham);
    fprintf('Blackman | %14.4f | %14.4f | %18.2f\n', main_b, total_b - main_b, slr_b);

    % Plot
    figure;
    plot(f, 20*log10(S_rect(1:Nfft/2)), 'k'); hold on;
    plot(f, 20*log10(S_hann(1:Nfft/2)), 'r');
    plot(f, 20*log10(S_hamming(1:Nfft/2)), 'g');
    plot(f, 20*log10(S_blackman(1:Nfft/2)), 'b');
    legend('Rectangular','Hann','Hamming','Blackman');
    xlim([f_ping-3000 f_ping+3000]); ylim([-100 5]);
    xlabel('Frequency (Hz)'); ylabel('Magnitude (dB)');
    title('Windowing Effects on Spectrum');
    grid on;

    Output 

    Window      | Mainlobe Power | Sidelobe Power | Sidelobe/Main (dB)
    ------------|----------------|----------------|--------------------
    Rectangular |         3.5771 |         4.9562 |               1.42
    Hann        |         4.3630 |         8.4370 |               2.86
    Hamming     |         4.2367 |         7.3928 |               2.42
    Blackman    |         4.4940 |        10.2410 |               3.58

     

     








Applications

  • Signal Processing: Analyzing frequency content of time-varying signals.

  • Communications: Evaluating spectrum occupancy in wireless systems.

  • Bioinformatics: Investigating periodicities in biological signals (e.g., EEG, ECG).

  • Seismology: Characterizing seismic wave frequencies.

     

    Further Reading

    1. Periodogram in MATLAB

Try Interactive Online Simulator to see the Effect

Contact Us

Name

Email *

Message *

Popular Posts

UGC NET Electronic Science Previous Year Question Papers with Solutions

Home / Engineering & Other Exams / UGC NET 2026 PYQ ⬇️ Download Papers and Solutions 📋 Exam Pattern 💡 Preparation Tips ❓ FAQs 📊 Exam Highlights: Electronic Science (88) Feature Details Junior Research Fellowship (JRF) ₹37,000 + HRA per month Eligibility M.Sc/M.Tech in Electronics (55%) Validity of Certificate JRF (3 Years) | Lectureship (Lifetime) 📥 Download UGC NET Electronics PDFs Complete collection of previous year question papers, answer keys and explanations for Subject Code 88. Start Downloading 📂 View All Question Papers June 2025 - Question Paper Download PDF June 2025 - Solved Paper + Explanation ...

UGC NET Electronic Science June 2025 Question Paper with Answer Key & Detailed Solutions

Home / UGC NET PYQ / June 2025 Solved UGC NET Electronic Science June 2025 Question Paper with Answer Key and Full Explanations 📥 Download Question Paper (PDF) 2025 2024 2023 2022 2021 2020 Explanations 1.  Answer: Option (3) For forming a p-type semiconductor, the dopant must be a trivalent impurity (three valence electrons) so that it creates acceptor levels and holes become the majority carriers. Among the given elements, boron (B) is a group-III element (trivalent). Arsenic (As) and phosphorus (P) are group-V (pentavalent) donors that produce n-type material, and germanium (Ge) is a group-IV element usually used as the semiconductor, not as an acceptor dopant. Hence, doping an intrinsic semiconductor with B produces a p-type semiconductor. 2.  Answer: Option (4) The ohmic resistance of a JFET at zero gate bias is given by the standard relation: R DS(on) = V P / I DSS ...

BER vs SNR for M-ary QAM, M-ary PSK, QPSK, BPSK, ...(MATLAB Code + Simulator)

Bit Error Rate (BER) & SNR Guide Analyze communication system performance with our interactive simulators and MATLAB tools. 📘 Theory 🧮 Simulators 💻 MATLAB Code 📚 Resources BER Definition SNR Formula BER Calculator MATLAB Comparison 📂 Explore M-ary QAM, PSK, and QPSK Topics ▼ 🧮 Constellation Simulator: M-ary QAM 🧮 Constellation Simulator: M-ary PSK 🧮 BER calculation for ASK, FSK, and PSK 🧮 Approaches to BER vs SNR What is Bit Error Rate (BER)? The BER indicates how many corrupted bits are received compared to the total number of bits sent. It is the primary figure of merit f...

Online Simulator for ASK, FSK, and PSK

Interactive Digital Signal Processing (DSP) Tutorial and Simulator for ASK, FSK, and BPSK modulation techniques. Try our new Digital Signal Processing Simulator!   •   Interactive ASK, FSK, and BPSK tools updated for 2025. Start Now Digital Modulation Visualizer: ASK, FSK, & BPSK Simulator Learn and visualize binary modulation techniques (ASK, FSK, BPSK) in real-time with adjustable carrier and sampling parameters. Perfect for DSP students and engineers. 📡 ASK Simulator 📶 FSK Simulator 🎚️ BPSK Simulator 📚 More Topics ASK Modulator FSK Modulator BPSK Modulator More Topics 1. ASK (Amplitude Shift Keying) Simulat...

UGC NET Electronic Science December 2024 Question Paper with Answer Key & Detailed Solutions

Home / UGC NET PYQ / June 2025 Solved UGC NET Electronic Science December 2024 Question Paper with Answer Key and Full Explanations 📥 Download Question Paper (PDF) 2025 2024 2023 2022 2021 2020 Q.1 Answer: Option (3) Q.2 Answer: Option (3) Solution 1. JMP SHORT LABEL Intrasegment (within the same code segment). Direct jump. ❌ Not intersegment indirect. 2. JMP 5000H:2000H Intersegment (far jump because both CS and IP are specified). Direct jump (address is explicitly given). ❌ Not indirect. 3. JMP [2000H] The destination address is taken from memory location 2000H. This is indirect. In 8086, a far indirect jump can use a memory operand containing both IP and CS (depending on operand size), making it an intersegment indirect jump. ✅ Correct answer. 4. JMP [BX] Indirect jump through memory addressed by BX. Usually intrasegment (near indirect jump). ❌ Not in...

Constellation Diagrams of ASK, PSK, and FSK (with MATLAB Code + Simulator)

Constellation Diagrams: ASK, FSK, and PSK Comprehensive guide to signal space representation, including interactive simulators and MATLAB implementations. 📘 Overview 🧮 Simulator ⚖️ Theory Q-function 📚 Resources 📂 Other Topics: M-ary PSK & QAM Diagrams ▼ 🧮 Simulator for M-ary PSK Constellation 🧮 Simulator for M-ary QAM Constellation BASK (Binary ASK) Modulation Transmits one of two signals: 0 or -√Eb, where Eb​ is the energy per bit. These signals represent binary 0 and 1. BFSK (Binary FSK) Modulation Transmits one of two signals: +√Eb​ (On the y-axis, the phas...

MATLAB Code for ASK, FSK, and PSK (with Online Simulator)

MATLAB Code for ASK, FSK, and PSK Comprehensive implementation of digital modulation and demodulation techniques with simulation results. 📘 Theory 📡 ASK Code 📶 FSK Code 🎚️ PSK Code 🕹️ Simulator 📚 Further Reading Amplitude Shift Frequency Shift Phase Shift Live Simulator ASK, FSK & PSK HomePage MATLAB Code MATLAB Code for ASK Modulation and Demodulation COPY % The code is written by SalimWireless.Com clc; clear all; close all; % Parameters Tb = 1; fc = 10; N_bits = 10; Fs = 100 * fc; Ts = 1/Fs; samples_per_bit = Fs * Tb; rng(10); binar...

Theoretical BER vs SNR for binary ASK, FSK, and PSK (with MATLAB Code + Simulator)

📘 Overview & Theory 🧮 MATLAB Codes 🧮 Q-function 📚 Further Reading Bit Error Rate (BER) Equations In ASK, noise directly affects the signal amplitude, making it the most vulnerable since the data is carried in amplitude changes. In FSK, data is represented by frequency variations, and because noise typically impacts amplitude more than frequency, FSK is more robust than ASK. In PSK, data is encoded in the signal phase, and BPSK specifically uses 180-degree phase shifts, creating the greatest separation between signal points and therefore achieving the lowest bit error rate (BER) for the same power level. BER formulas for ASK, FSK, and PSK modulation schemes. ASK BER = 0.5 × erfc(0.5 × √SNR) FSK BER = 0.5 × erfc(√(SNR / 2)) PSK BER = 0.5 × erfc(√SNR) ...