Numerous texts are available to explain the basics of Discrete Fourier Transform and its very efficient implementation – Fast Fourier Transform (FFT). Often we are confronted with the need to generate simple, standard signals (sine, cosine, Gaussian pulse, square wave, isolated rectangular pulse, exponential decay, chirp signal) for simulation purpose. I intend to show (in a series of articles) how these basic signals can be generated in Matlab and how to represent them in frequency domain using FFT.
This article is part of the book Digital Modulations using Matlab : Build Simulation Models from Scratch, ISBN: 978-1521493885 available in ebook (PDF) format (click here) and Paperback (hardcopy) format (click here)
Wireless Communication Systems in Matlab, ISBN: 978-1720114352 available in ebook (PDF) format (click here) and Paperback (hardcopy) format (click here).
Rectangular pulse: mathematical description
An isolated rectangular pulse of amplitude A and duration T is represented mathematically as
where
The Fourier transform of isolated rectangular pulse g(t) is
where, the sinc function is given by
Thus, the Fourier Transform pairs are
The Fourier Transform describes the spectral content of the signal at various frequencies. For a given signal g(t), the Fourier Transform is given by
where, the absolute value gives the magnitude of the frequency components (amplitude spectrum) and are their corresponding phase (phase spectrum) . For the rectangular pulse, the amplitude spectrum is given as
The amplitude spectrum peaks at f=0 with value equal to AT. The nulls of the spectrum occur at integral multiples of 1/T, i.e, ( )
Generating an isolated rectangular pulse in Matlab:
An isolated rectangular pulse of unit amplitude and width w (the factor T in equations above ) can be generated easily with the help of in-built function – rectpuls(t,w) command in Matlab. As an example, a unit amplitude rectangular pulse of duration is generated.
fs=500; %sampling frequency
T=0.2; %width of the rectangule pulse in seconds
t=-0.5:1/fs:0.5; %time base
x=rectpuls(t,T); %generating the square wave
plot(t,x,'k');
title(['Rectangular Pulse width=', num2str(T),'s']);
xlabel('Time(s)');
ylabel('Amplitude');
Amplitude spectrum using FFT:
Matlab’s FFT function is utilized for computing the Discrete Fourier Transform (DFT). The magnitude of FFT is plotted. From the following plot, it can be noted that the amplitude of the peak occurs at f=0 with peak value . The nulls in the spectrum are located at ().
L=length(x);
NFFT = 1024;
X = fftshift(fft(x,NFFT)); %FFT with FFTshift for both negative & positive frequencies
f = fs*(-NFFT/2:NFFT/2-1)/NFFT; %Frequency Vector
figure;
plot(f,abs(X)/(L),'r');
title('Magnitude of FFT');
xlabel('Frequency (Hz)')
ylabel('Magnitude |X(f)|');
Power spectral density (PSD) using FFT:
The distribution of power among various frequency components is plotted next. The first plot shows the double-side Power Spectral Density which includes both positive and negative frequency axis. The second plot describes the PSD only for positive frequency axis (as the response is just the mirror image of negative frequency axis).
figure;
Pxx=X.*conj(X)/(L*L); %computing power with proper scaling
plot(f,10*log10(Pxx),'r');
title('Double Sided - Power Spectral Density');
xlabel('Frequency (Hz)')
ylabel('Power Spectral Density- P_{xx} dB/Hz');
X = fft(x,NFFT);
X = X(1:NFFT/2+1);%Throw the samples after NFFT/2 for single sided plot
Pxx=X.*conj(X)/(L*L);
f = fs*(0:NFFT/2)/NFFT; %Frequency Vector
plot(f,10*log10(Pxx),'r');
title('Single Sided - Power Spectral Density');
xlabel('Frequency (Hz)')
ylabel('Power Spectral Density- P_{xx} dB/Hz');
Magnitude and phase spectrum:
The phase spectrum of the rectangular pulse manifests as series of pulse trains bounded between 0 and , provided the rectangular pulse is symmetrically centered around sample zero. This is explained in the reference here and the demo below.
clearvars;
x = [ones(1,7) zeros(1,127-13) ones(1,6)];
subplot(3,1,1); plot(x,'k');
title('Rectangular Pulse'); xlabel('Sample#'); ylabel('Amplitude');
NFFT = 127;
X = fftshift(fft(x,NFFT)); %FFT with FFTshift for both negative & positive frequencies
f = (-NFFT/2:NFFT/2-1)/NFFT; %Frequency Vector
subplot(3,1,2); plot(f,abs(X),'r');
title('Magnitude Spectrum'); xlabel('Frequency (Hz)'); ylabel('|X(f)|');
subplot(3,1,3); plot(f,atan2(imag(X),real(X)),'r');
title('Phase Spectrum'); xlabel('Frequency (Hz)'); ylabel('\angle X(f)');
Rate this article:
Hello,
It would be great help for us(learners from your material) if you can explain in detail why you choose the frequency f in this manner. What is the NFFT? and why and how you made f.
L=length(x);
NFFT = 1024;
X = fftshift(fft(x,NFFT)); %FFT with FFTshift for both negative & positive frequencies
f = fs*(-NFFT/2:NFFT/2-1)/NFFT; %Frequency Vector
Thank you very much in advance.
regards
tilkesh
Hello Tilkesh,
I have explained some of the related details in this article. Link below
How to Interpret FFT results – complex DFT, frequency bins and FFTShift
https://www.gaussianwaves.com/2015/11/interpreting-fft-results-complex-dft-frequency-bins-and-fftshift/
I appreciate your time, efforts and contribution to the knowledge community. Your work is highly valuable for students and researchers who wants to learn this subject and apply in their field.
Hi, thank for your posts in this website.
I have a question… Why the magnitude of the spectrum does not touch the zero in the points in which the sinc function (that is the fourier transform of a rect pulse) should be null?
Is that due to the fact that we are performing a DFT?
And if we plot the phase spectrum, that of a sinc should be a train of rect pulses between 0 and -pi when the sinc is negative, what information do we have instead?
Thanks.
The magnitude spectrum does not touch zero due to the relationship between the FFT length that controls the bin centers and the points where the sinc function supposed to touch zero. If the FFT length is adjusted appropriately according to the width of the rect pulse, the magnitude spectrum will touch zero at expected null places.
Phase spectrum depends on how the input pulse is presented to the FFT. It is explained in the reference here : http://www.dspguide.com/ch11/2.htm
Check how to get phase spectrum as you have mentioned in your question. I have provided this additional information in the post above.
Hi!
First of all, thanks a lot for your explanation of FFT using MATLAB. It has been quite helpful for me. Anyway, there is a little question i would appreciate your help.
I am using the Rect function just for training since I have to use Fourier transforms to analize a diffraction pattern problem. In this case, it is important for me to recover the sign of the sinc function (i.e. those frequencies where it is negative) and plotting the ABS value makes me to loose this information. Is there any way to obtain a SINC fuction and not just a |sinc|?
Thank you
FFT encodes information on exponential basis functions, so both real and imaginary part of the FFT output contains all valuable information. FFT gives result in complex format.
Information is presented in polar form : magnitude and the phase.
Magnitudes represent intensity deviation from zero and hence can have only positive values. If you would like to have negative values in magnitude (its against formal definition of magnitude to carry negative values), further processing needs to be done.
These pages may help in better understanding
http://www.dspguide.com/ch11/2.htm