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[[Category:problem solving]]
 
[[Category:problem solving]]
 
= Compute the energy  <math class="inline">E_\infty</math> and the power  <math class="inline">P_\infty</math> of the following continuous-time signal=
 
= Compute the energy  <math class="inline">E_\infty</math> and the power  <math class="inline">P_\infty</math> of the following continuous-time signal=
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===Answer 1===
 
===Answer 1===
b) <math class="inline">E_{\infty}=\lim_{T\rightarrow \infty}\int_{-T}^T |e^{(2jt)}|^2 dx = \lim_{T\rightarrow \infty}\int_{-T}^T |(cos(2t) + j*sin(2t))|^2 dx = \lim_{T\rightarrow \infty}\int_{-T}^T {\sqrt{(cos(2t))^2 + (sin(2t))^2}}^2 dx = \lim_{T\rightarrow \infty}\int_{-T}^T 1 dx = \lim_{T\rightarrow \infty} t \Big| ^T _{-T} </math>
+
<math>
 +
\begin{align}
 +
E_{\infty}&=\lim_{T\rightarrow \infty}\int_{-T}^T |e^{(2jt)}|^2 dx \\
 +
&= \lim_{T\rightarrow \infty}\int_{-T}^T |(cos(2t) + j*sin(2t))|^2 dx \\
 +
&= \lim_{T\rightarrow \infty}\int_{-T}^T {\sqrt{(cos(2t))^2 + (sin(2t))^2}}^2 dx\\
 +
& = \lim_{T\rightarrow \infty}\int_{-T}^T 1 dx \\
 +
&= \lim_{T\rightarrow \infty} t \Big| ^T _{-T}\\
 +
&=\infty.
 +
\end{align}
 +
</math>
  
<math class="inline">E_{\infty} = \infty</math>
+
So <math class="inline">E_{\infty} = \infty</math>.
  
<math class="inline">P_{\infty}=\lim_{T\rightarrow \infty} {1 \over {2T}} \int_{-T}^T |e^{(2jt)}|^2 dx = \lim_{T\rightarrow \infty} {1 \over {2T}} \int_{-T}^T 1 dx = \lim_{T\rightarrow \infty} {1 \over {2T}} t \Big| ^T _{-T} = \lim_{T\rightarrow \infty} {1 \over {2T}} T - {1 \over {2T}} (-T) = \lim_{T\rightarrow \infty} {1 \over {2}} + {1 \over {2}} = 1</math>
+
<math>
 +
\begin{align}
 +
P_{\infty}&=\lim_{T\rightarrow \infty} {1 \over {2T}} \int_{-T}^T |e^{(2jt)}|^2 dx \\
 +
&= \lim_{T\rightarrow \infty} {1 \over {2T}} \int_{-T}^T 1 dx \\
 +
& = \lim_{T\rightarrow \infty} {1 \over {2T}} t \Big| ^T _{-T} \\
 +
& = \lim_{T\rightarrow \infty} {1 \over {2T}} T - {1 \over {2T}} (-T)\\
 +
& = \lim_{T\rightarrow \infty} {1 \over {2}} + {1 \over {2}} \\
 +
&= 1
 +
\end{align}
 +
</math>
  
<math class="inline">P_{\infty} = 1</math>
+
So <math class="inline">P_{\infty} = 1 </math>.
  
 
<math>P_\infty</math> is larger than 0, so <math>E_\infty</math> should be infinity, and it is.
 
<math>P_\infty</math> is larger than 0, so <math>E_\infty</math> should be infinity, and it is.

Revision as of 16:02, 12 January 2011

Compute the energy $ E_\infty $ and the power $ P_\infty $ of the following continuous-time signal

$ x(t)= e^{2jt} $

What properties of the complex magnitude can you use to check your answer?


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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

$ \begin{align} E_{\infty}&=\lim_{T\rightarrow \infty}\int_{-T}^T |e^{(2jt)}|^2 dx \\ &= \lim_{T\rightarrow \infty}\int_{-T}^T |(cos(2t) + j*sin(2t))|^2 dx \\ &= \lim_{T\rightarrow \infty}\int_{-T}^T {\sqrt{(cos(2t))^2 + (sin(2t))^2}}^2 dx\\ & = \lim_{T\rightarrow \infty}\int_{-T}^T 1 dx \\ &= \lim_{T\rightarrow \infty} t \Big| ^T _{-T}\\ &=\infty. \end{align} $

So $ E_{\infty} = \infty $.

$ \begin{align} P_{\infty}&=\lim_{T\rightarrow \infty} {1 \over {2T}} \int_{-T}^T |e^{(2jt)}|^2 dx \\ &= \lim_{T\rightarrow \infty} {1 \over {2T}} \int_{-T}^T 1 dx \\ & = \lim_{T\rightarrow \infty} {1 \over {2T}} t \Big| ^T _{-T} \\ & = \lim_{T\rightarrow \infty} {1 \over {2T}} T - {1 \over {2T}} (-T)\\ & = \lim_{T\rightarrow \infty} {1 \over {2}} + {1 \over {2}} \\ &= 1 \end{align} $

So $ P_{\infty} = 1 $.

$ P_\infty $ is larger than 0, so $ E_\infty $ should be infinity, and it is. --Cmcmican 19:50, 12 January 2011 (UTC)

Answer 2

write it here.

Answer 3

write it here.


Back to ECE301 Spring 2011 Prof. Boutin

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Questions/answers with a recent ECE grad

Ryne Rayburn