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− | = Practice Question on the Properties of the Continuous-time Fourier Transform = | + | = [[:Category:Problem_solving|Practice Question]] on the Properties of the Continuous-time Fourier Transform = |
Let x(t) be a continuous time signal with Fourier transform <math class="inline">{\mathcal X} (\omega) </math>. | Let x(t) be a continuous time signal with Fourier transform <math class="inline">{\mathcal X} (\omega) </math>. | ||
Line 36: | Line 36: | ||
</math> | </math> | ||
=== Answer 2 === | === Answer 2 === | ||
− | + | <math> | |
+ | \begin{align} | ||
+ | {\mathcal F} \left( x(3t+7) \right) &= \int_{-\infty}^\infty x(3t+7) e^{-j\omega t} dt \\ | ||
+ | &= \int_{-\infty}^\infty x(u) e^{-j\omega \frac{(u-7)}{3}} \frac{du}{3}, \text{ (letting }u=3t+7), \\ | ||
+ | &= \frac{1}{3} \int_{-\infty}^\infty x(u)e^{-\frac{j\omega u}{3}}e^{\frac{7j\omega}{3}} du\\ | ||
+ | &= \frac{e^{\frac{7j\omega}{3}}}{3}\int_{-\infty}^\infty x(u)e^{-\frac{j\omega u}{3}} du \\ | ||
+ | &= \frac{e^{\frac{7j\omega}{3}}}{3} \mathcal{X}(\omega) | ||
+ | \end{align} | ||
+ | </math> | ||
+ | --[[User:Ekhall|Ekhall]] 11:45, 2 March 2011 (UTC) | ||
+ | |||
+ | :<span style="color:red">Instructor's note: You should replace <math class="inline">\mathcal{X}(\omega)</math> by <math class="inline">\mathcal{X}(\frac{\omega}{3})</math>. </span> | ||
=== Answer 3 === | === Answer 3 === | ||
Write it here. | Write it here. | ||
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[[2011_Spring_ECE_301_Boutin|Back to ECE301 Spring 2011 Prof. Boutin]] | [[2011_Spring_ECE_301_Boutin|Back to ECE301 Spring 2011 Prof. Boutin]] |
Latest revision as of 10:27, 11 November 2011
Contents
Practice Question on the Properties of the Continuous-time Fourier Transform
Let x(t) be a continuous time signal with Fourier transform $ {\mathcal X} (\omega) $.
We have seen the time-shifting property of the Fourier transform:
$ {\mathcal F} \left( x(t-t_0) \right) = e^{-j \omega t_0} {\mathcal X} (\omega) $
which gives us an expression for the Fourier transform of $ y(t)=x(t-t_0) $ in terms of $ {\mathcal X} (\omega) $. Note that, to prove this property, one can proceed as follows:
$ \begin{align} {\mathcal F} \left( x(t-t_0) \right) &= \int_{-\infty}^\infty x(t-t_0) e^{-j\omega t} dt \\ &= \int_{-\infty}^\infty x(u) e^{-j\omega (u+t_0)} du, \text{ (letting }u=t-t_0), \\ &= e^{-j\omega t_0} \int_{-\infty}^\infty x(u) e^{-j\omega u} du \\ &= e^{-j\omega t_0} {\mathcal X} (\omega). \end{align} $
Using a similar approach as above, derive an expression for the Fourier transform of y(t)=x(3t+7) in terms of $ {\mathcal X} (\omega) $.
You will receive feedback from your instructor and TA directly on this page. Other students are welcome to comment/discuss/point out mistakes/ask questions too!
Answer 1
Instructor's hint: You should start like this
$ \begin{align} {\mathcal F} \left( x(3t+7) \right) &= \int_{-\infty}^\infty x(3t+7) e^{-j\omega t} dt \\ &= \int_{-\infty}^\infty x(u) e^{-j\omega \frac{(u-7)}{3}} \frac{du}{3}, \text{ (letting }u=3t+7), \\ &= ... \end{align} $
Answer 2
$ \begin{align} {\mathcal F} \left( x(3t+7) \right) &= \int_{-\infty}^\infty x(3t+7) e^{-j\omega t} dt \\ &= \int_{-\infty}^\infty x(u) e^{-j\omega \frac{(u-7)}{3}} \frac{du}{3}, \text{ (letting }u=3t+7), \\ &= \frac{1}{3} \int_{-\infty}^\infty x(u)e^{-\frac{j\omega u}{3}}e^{\frac{7j\omega}{3}} du\\ &= \frac{e^{\frac{7j\omega}{3}}}{3}\int_{-\infty}^\infty x(u)e^{-\frac{j\omega u}{3}} du \\ &= \frac{e^{\frac{7j\omega}{3}}}{3} \mathcal{X}(\omega) \end{align} $ --Ekhall 11:45, 2 March 2011 (UTC)
- Instructor's note: You should replace $ \mathcal{X}(\omega) $ by $ \mathcal{X}(\frac{\omega}{3}) $.
Answer 3
Write it here.