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[[Category:problem solving]]
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[[Category:ECE301]]
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[[Category:ECE]]
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[[Category:Fourier series]]
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[[Category:signals and systems]]
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== Example of Computation of Fourier series of a CT SIGNAL ==
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A [[Signals_and_systems_practice_problems_list|practice problem on "Signals and Systems"]]
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----
 
==Problem==
 
==Problem==
 
Find the Fourier series coefficients of a CT signal.
 
Find the Fourier series coefficients of a CT signal.
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We know
 
We know
  
<math>a_k e^{jkw_0t}</math>
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<math>a_k e^{jkw_0t}</math> corresponds to <math>\frac{3}{2}e^{j2t}</math> and <math>\frac{3}{2}e^{-j2t}</math>
 
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corresponds to
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<math>\frac{3}{2}e^{j2t}</math> and <math>\frac{3}{2}e^{-j2t}</math>
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and since <math>w_0 = 1</math>, then we can conclude
 
and since <math>w_0 = 1</math>, then we can conclude
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and
 
and
  
<math>a_k = 0</math> for <math>K \neq 2, -2</math>
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<math>a_k = 0 \!</math> for <math>K \neq 2, -2</math>
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----
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[[Signals_and_systems_practice_problems_list|Back to Practice Problems on Signals and Systems]]

Latest revision as of 10:54, 16 September 2013

Example of Computation of Fourier series of a CT SIGNAL

A practice problem on "Signals and Systems"


Problem

Find the Fourier series coefficients of a CT signal.

I chose the signal $ x(t) = 3cos(2t) $.

Fourier Series Coefficients

The Fourier series of a CT signal can be found by:

$ x(t) = \sum_{n=-\infty}^\infty a_k e^{jkw_0t} $

Fourier series coefficients can be found with the equation:

$ a_k = \frac{1}{T} \int_{0}^{T} x(t)e^{-jkw_0t} \,\ dt $

However, in the case of sinusoidal waves, the coefficients can be found more simply by applying Euler's formula to solve for the Fourier series and take the coefficients from that.

$ x(t) = 3cos(2t) = 3(\frac{e^{j2t}}{2}+\frac{e^{-j2t}}{2}) $

$ = \frac{3}{2}e^{j2t}+\frac{3}{2}e^{-j2t} $

And so, we know that our coefficients are both $ \frac{3}{2} $. Now, we need to find which $ a_k $s these belong to.

Knowing $ T $ is $ 2\pi $, we can find $ w_0 $.

$ w_0 = \frac{2\pi}{T} = \frac{2\pi}{2\pi} = 1 $

Finding the corresponding $ k $s should be easy.

We know

$ a_k e^{jkw_0t} $ corresponds to $ \frac{3}{2}e^{j2t} $ and $ \frac{3}{2}e^{-j2t} $

and since $ w_0 = 1 $, then we can conclude

$ a_2 = \frac{3}{2} $

and

$ a_{-2} = \frac{3}{2} $

and

$ a_k = 0 \! $ for $ K \neq 2, -2 $


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