m
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<math>  \Rightarrow ~~~~~~~= \frac {e^{j2t} - 1}{jt\pi} - \frac {1 - e^{-j2t}}{jt\pi} </math>
 
<math>  \Rightarrow ~~~~~~~= \frac {e^{j2t} - 1}{jt\pi} - \frac {1 - e^{-j2t}}{jt\pi} </math>
  
<math>  \Rightarrow ~~~~~~~= \left (  \frac {e^{j2t} + e^{-j2t) - 2}{jt\pi} \right ) </math>
+
<math>  \Rightarrow ~~~~~~~= \left (  \frac {e^{j2t} + e^{-j2t} - 2}{jt\pi} \right ) </math>

Revision as of 19:09, 1 July 2008

Solution to Prob 4.4b

Its given that X(jw) =

$ ~2, ~~0 \le \omega \le 2 $

$ -2, ~~-2 \le \omega < 0 $

$ ~0, ~~|\omega| > 2 $

$ \therefore x_2(t) = \frac {1}{2\pi} \int_{-\infty}^{\infty} X_2(j\omega) e^{jt\omega}\,d\omega $

$ \Rightarrow ~~~~~~~= \frac {1}{2\pi} \int_{0}^{2} 2 e^{jt\omega}\,d\omega + \frac {1}{2\pi} \int_{-2}^{0} (-2) e^{jt\omega}\,d\omega $


$ \Rightarrow ~~~~~~~= \frac {e^{j2t} - 1}{jt\pi} - \frac {1 - e^{-j2t}}{jt\pi} $

$ \Rightarrow ~~~~~~~= \left ( \frac {e^{j2t} + e^{-j2t} - 2}{jt\pi} \right ) $

Alumni Liaison

Abstract algebra continues the conceptual developments of linear algebra, on an even grander scale.

Dr. Paul Garrett