FFT of a Zero-Padded Sinusoid
FFT of a Simple Sinusoid
Spectrum Analysis of a Sinusoid
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Now let's increase the frequency in the above example by one-half of a bin:
% Example 2 = Example 1 with frequency between bins
f = 0.25 + 0.5/N; % Move frequency up 1/2 bin
x = cos(2*pi*n*f*T); % Signal to analyze
X = fft(x); % Spectrum
... % See Example 1 for plots and such
Figure:
Sinusoid at Frequency
. a) Time waveform. b) Magnitude spectrum. c) DB
magnitude spectrum.
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The resulting magnitude spectrum is shown in Fig. 8.2b and c.
At this frequency, we get extensive ``spectral leakage'' into all the
bins. To get an idea of where this is coming from, let's look at the
periodic extension of the time waveform:
% Plot the periodic extension of the time-domain signal
plot([x,x],'--ok');
title('Time Waveform Repeated Once');
xlabel('Time (samples)'); ylabel('Amplitude');
The result is shown in Fig. 8.3. Note the ``glitch'' in the
middle where the signal begins its forced repetition.
Figure:
Time waveform repeated to show
discontinuity introduced by periodic extension (see midpoint).
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FFT of a Zero-Padded Sinusoid
FFT of a Simple Sinusoid
Spectrum Analysis of a Sinusoid
Contents
Global Contents
Global Index
  Index
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``Mathematics of the Discrete Fourier Transform (DFT)'',
by Julius O. Smith III,
W3K Publishing, 2003, ISBN 0-9745607-0-7.
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Copyright © 2003-10-09 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),
Stanford University
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