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:<span style="color:green">Instructor's comments: Guessing the answer and proving it using the inverse Fourier transform is a good trick. One could also obtain this Fourier transform using the duality property and your previous answer. -pm </span>
 
:<span style="color:green">Instructor's comments: Guessing the answer and proving it using the inverse Fourier transform is a good trick. One could also obtain this Fourier transform using the duality property and your previous answer. -pm </span>
 
===Answer 2===
 
===Answer 2===
Write it here.
+
<math> X(f)=\int_{-\infty}^{\infty} x(t)e^{-j2\pi ft} dt
 +
          =\int_{-\infty}^{\infty} rect(t)e^{-j2\pi ft} dt
 +
          =\int_{-\frac{1}{2}}^{\frac{1}{2}} e^{-j2\pi ft} dt
 +
</math>
 +
 
 +
<math> = -\frac{e^{-j2\pi ft}}{-j2\pi f}
 +
</math>
 +
integrating from -0.5 to +0.5.
 +
<math> = \frac{e^{-j\pi f} - e^{j\pi f}}{-j2\pi f}
 +
      = \frac{sin(\pi f)}{\pi f}
 +
</math>
 +
 
 +
 
 +
For y(t), we know that
 +
 
 +
<math> y(t) = \int_{-\infty}^{\infty} Y(f)e^{j2\pi ft} df
 +
</math>
 +
 +
<math> y(t)= \frac{ \sin ( \pi t )}{\pi t}
 +
      = \frac{e^{-j\pi t} - e^{j\pi t}}{\pi t}  </math>
 +
 
 +
For the above equation to be true,
 +
 
 +
<math> Y(f) = \frac{\delta(f - \frac{1}{2})}{\pi t} - \frac{\delta(f + \frac{1}{2})}{\pi t}
 +
</math>
 +
 
 
===Answer 3===
 
===Answer 3===
 
write it here.
 
write it here.
 
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Revision as of 14:31, 6 September 2011

Continuous-time Fourier transform computation (in terms of frequency f in hertz)

Compute the Continuous-time Fourier transform of the two following functions:

$ x(t)= \text{rect}(t) = \left\{ \begin{array}{ll} 1, & \text{ if } |t|<\frac{1}{2}\\ 0, & \text{ else} \end{array} \right. $

$ y(t)= \frac{ \sin ( \pi t )}{\pi t} $

Justify your answer.


Share your answers below

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Answer 1

Fourier Transform of rect(t):

$ X(f)=\int_{-\infty}^{\infty} x(t)e^{-j2\pi ft} dx =\int_{\frac{-1}{2}}^{\frac{1}{2}} e^{-j2\pi ft} dx =\frac{e^{-j2\pi ft}}{-j2\pi f} $ from t=-1/2 to t=1/2

$ =\frac{e^{-j\pi f}-e^{j\pi f}}{-j2\pi f} =\frac{sin(\pi f)}{\pi f} $

Instructor's comments: Technically, you should look at the case f=0 separately, because your solution involves a division by f. -pm

Fourier Transform of $ \frac{sin(\pi t)}{\pi t} $:

Guess: $ X(f)=rect(t) $

Proof:

$ x(t)=\int_{-\infty}^{\infty} X(f)e^{j2\pi ft} df =\int_{\frac{-1}{2}}^{\frac{1}{2}} e^{j2\pi ft} df =\frac{e^{j2\pi ft}}{j2\pi t} $ from f=-1/2 to f=1/2

$ =\frac{e^{j\pi t}-e^{j\pi t}}{j2\pi t} =\frac{sin(\pi t)}{\pi t} $

Instructor's comments: Guessing the answer and proving it using the inverse Fourier transform is a good trick. One could also obtain this Fourier transform using the duality property and your previous answer. -pm

Answer 2

$ X(f)=\int_{-\infty}^{\infty} x(t)e^{-j2\pi ft} dt =\int_{-\infty}^{\infty} rect(t)e^{-j2\pi ft} dt =\int_{-\frac{1}{2}}^{\frac{1}{2}} e^{-j2\pi ft} dt $

$ = -\frac{e^{-j2\pi ft}}{-j2\pi f} $ integrating from -0.5 to +0.5. $ = \frac{e^{-j\pi f} - e^{j\pi f}}{-j2\pi f} = \frac{sin(\pi f)}{\pi f} $


For y(t), we know that

$ y(t) = \int_{-\infty}^{\infty} Y(f)e^{j2\pi ft} df $

$ y(t)= \frac{ \sin ( \pi t )}{\pi t} = \frac{e^{-j\pi t} - e^{j\pi t}}{\pi t} $

For the above equation to be true,

$ Y(f) = \frac{\delta(f - \frac{1}{2})}{\pi t} - \frac{\delta(f + \frac{1}{2})}{\pi t} $

Answer 3

write it here.


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