(New page: The overall response for this system is <math>f(t) = tf(-t)</math> To relate to the systems that were already use in example <math>\cos(2t) = \frac{e^{i2t}+e^{-i2t}}{2}</math> <math>\...)
 
 
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<math>\cos(2t) = \frac{e^{i2t}+e^{-i2t}}{2}</math>
 
<math>\cos(2t) = \frac{e^{i2t}+e^{-i2t}}{2}</math>
  
<math>\frac{e^{i2t}+e^{-i2t}}{2}=\frac{te^{-i2t}+te^{i2t}}{2} = t\frac{e^{-i2t}+e^{i2t}}{2}</math>
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So when the signal is run through the system the following is what is produced
 +
 
 +
<math>\frac{e^{i2t}+e^{-i2t}}{2}=\frac{te^{-i2t}+te^{i2t}}{2} = t\frac{e^{-i2t}+e^{i2t}}{2} = t\cos(2t)</math>

Latest revision as of 08:09, 19 September 2008

The overall response for this system is

$ f(t) = tf(-t) $

To relate to the systems that were already use in example

$ \cos(2t) = \frac{e^{i2t}+e^{-i2t}}{2} $

So when the signal is run through the system the following is what is produced

$ \frac{e^{i2t}+e^{-i2t}}{2}=\frac{te^{-i2t}+te^{i2t}}{2} = t\frac{e^{-i2t}+e^{i2t}}{2} = t\cos(2t) $

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

Dr. Paul Garrett