Revision as of 03:26, 2 December 2018 by Cdube (Talk | contribs)


Moving between the Time Domain and Frequency Domain

Summary

This is a summary of how to move between the Time Domain and Frequency Domain, and an example of how one can solve for the output of a system via either the time domain or frequency domain. You will come to the same answer.

The relationship is summarized as follows:

$ x(t)*h(t)=y(t) $

$ \phantom{a} \downarrow \phantom{aaa} \downarrow \phantom{aaa} \downarrow \phantom{aaa} \textrm{Fourier transform} $

$ X(w) H(w) = Y(w) $


Thus, given the signal x(t) and the unit impulse response h(t), one can either directly calculate the response y(t) via convolution in the time domain, or one can apply the Fourier transform to x(t) and y(t) to move into the Fourier domain. There, the Fourier transforms, X(ω) and H(ω) respectively, can be multiplied together to obtain Y(ω), and Y(ω) can be inverse Fourier transformed to find y(t). Though this process requires more steps, its computations are easier. Here is a CT example of how each of these two methods can be used to find y(t).


Given: a signal x(t) = cos(2π440t), and the unit impulse response h(t) = δ(t-7) Find: the system response y(t)

Method 1: Exclusively Time Domain

$ y(t) = x(t) * h(t) $

$ \phantom{aaaa} = \int_{-\infty}^{\infty} x(\tau) h(t - \tau) d\tau $ by the definition of convolution

$ \phantom{aaaa} = \int_{-\infty}^{\infty} \left( \frac{1}{2}e^{j2\pi440\tau} + \frac{1}{2}e^{-j2\pi440\tau} \right) \delta\left ( t - \tau - 7 \right ) d\tau $ applying the Fourier series representation of cosine

$ \phantom{aaaa} = \int_{-\infty}^{\infty} \left( \frac{1}{2}e^{j2\pi440(t-7)} + \frac{1}{2}e^{-j2\pi440(t-7)} \right) \delta\left ( t - \tau - 7 \right ) d\tau $ because the result is only non-zero when τ = t - 7

$ \phantom{aaaa} = \left( \frac{1}{2}e^{j2\pi440(t-7)} + \frac{1}{2}e^{-j2\pi440(t-7)} \right) \int_{-\infty}^{\infty} \delta\left ( t - \tau - 7 \right ) d\tau $

$ \phantom{aaaa} = \frac{1}{2}e^{j2\pi440(t-7)} + \frac{1}{2}e^{-j2\pi440(t-7)} $

$ \phantom{aaaa} = \cos \left (2 \pi 440(t - 7) \right ) $


Method 2: Using the Frequency Domain

$ Y(\omega) = X(\omega) H(\omega) $

Fourier Transform of x(t): Because x(t) is a periodic function, the traditional equation to calculate its Fourier transform should not be applied. We will guess the Fourier transform, and apply the equation for the inverse Fourier transform to confirm that our guess is correct.

guess: $ [[ 2018 Fall ECE 301 Boutin|Back to 2018 Fall ECE 301 Boutin]] $

Alumni Liaison

Ph.D. on Applied Mathematics in Aug 2007. Involved on applications of image super-resolution to electron microscopy

Francisco Blanco-Silva