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Given the system <math>y(t) = 2x(t+3)\,</math>
 
Given the system <math>y(t) = 2x(t+3)\,</math>
  
<math> x(t)= \2delta(t+3) </math>
+
<math> x(t)= 2\delta(t+3) </math>
  
 
Then find the response to <math>x(t) = cos(4t) + sin(2t)\,</math>
 
Then find the response to <math>x(t) = cos(4t) + sin(2t)\,</math>
 +
 +
<math>x(t)=\frac{1}{2}e^{j4\pi t}+\frac{1}{2}e^{-j4\pi t}+\frac{1}{2j}e^{j2\pi t}+\frac{-1}{2j}e^{-j2\pi t}</math>
 +
 +
<math>H(j\omega)=\int_{-\infty}^\infty h(\tau)e^{-j\omega\tau}d\tau</math>
 +
 +
<math>H(j\omega)=\int_{-\infty}^\infty (2\delta(\tau+3))e^{-j\omega\tau}d\tau</math>
 +
 +
y(t) = x(t)*H(t)
 +
 +
<math>y(t) = (2e^{3j\omega})*(\frac{1}{2}e^{j4\pi t}+\frac{1}{2}e^{-j4\pi t}+\frac{1}{2j}e^{j2\pi t}+\frac{-1}{2j}e^{-j2\pi t})</math>

Latest revision as of 17:08, 26 September 2008

Given the system $ y(t) = 2x(t+3)\, $

$ x(t)= 2\delta(t+3) $

Then find the response to $ x(t) = cos(4t) + sin(2t)\, $

$ x(t)=\frac{1}{2}e^{j4\pi t}+\frac{1}{2}e^{-j4\pi t}+\frac{1}{2j}e^{j2\pi t}+\frac{-1}{2j}e^{-j2\pi t} $

$ H(j\omega)=\int_{-\infty}^\infty h(\tau)e^{-j\omega\tau}d\tau $

$ H(j\omega)=\int_{-\infty}^\infty (2\delta(\tau+3))e^{-j\omega\tau}d\tau $

y(t) = x(t)*H(t)

$ y(t) = (2e^{3j\omega})*(\frac{1}{2}e^{j4\pi t}+\frac{1}{2}e^{-j4\pi t}+\frac{1}{2j}e^{j2\pi t}+\frac{-1}{2j}e^{-j2\pi t}) $

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Ryne Rayburn