(New page: ==CT Signal & its Fourier coefficients== Lets define the signal <math>\ x(t) = (1+2j)cos(t)+3sin(2t) </math>)
 
(CT Signal & its Fourier coefficients)
 
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Lets define the signal
 
Lets define the signal
  
<math>\ x(t) = (1+2j)cos(t)+3sin(2t) </math>
+
<math>\ x(t) = (1+2j)cos(t)+5sin(4t) </math>
 +
 
 +
Knowing that its Fourier series is
 +
 
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<math>\ x(t) = (1+2j)(\frac{e^{jt} + e^{-jt}}{2}) + 5(\frac{e^{j4t} - e^{-j4t}}{2j}) </math>
 +
 
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We simplify
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<math>\ x(t) = \frac{1+2j}{2} e^{jt} + \frac{1+2j}{2} e^{-jt} + \frac{5}{2j}e^{j4t} - \frac{5}{2j}e^{-j4t} </math>

Latest revision as of 21:38, 23 September 2008

CT Signal & its Fourier coefficients

Lets define the signal

$ \ x(t) = (1+2j)cos(t)+5sin(4t) $

Knowing that its Fourier series is

$ \ x(t) = (1+2j)(\frac{e^{jt} + e^{-jt}}{2}) + 5(\frac{e^{j4t} - e^{-j4t}}{2j}) $

We simplify

$ \ x(t) = \frac{1+2j}{2} e^{jt} + \frac{1+2j}{2} e^{-jt} + \frac{5}{2j}e^{j4t} - \frac{5}{2j}e^{-j4t} $

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

Dr. Paul Garrett