(New page: <font size="3">Let <math>x(t)=cos(4 \pi t) + sin(6 \pi t)</math> Then <math>h(t) =</math> </font>)
 
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<font size="3">Let <math>x(t)=cos(4 \pi t) + sin(6 \pi t)</math>
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<font size="3">Let <math>y(t)=\int_{-\infty}^{\infty}2x(t)dt</math>
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Then <math>h(t) =2u(t)</math>
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And <math>H(s) = \int_{-\infty}^{\infty}h(t)e^{-st}dt</math>
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<math>=\int_{-\infty}^{\infty}2u(t)e^{-st}dt</math>
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<math>=\int_{0}^{\infty}2e^{-st}dt</math>
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<math>=(\frac{-2}{s}e^{-st})|_{0}^{\infty}</math>
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<math>=\frac{2}{s}</math>
  
Then <math>h(t) =</math>
 
 
</font>
 
</font>

Revision as of 12:50, 24 September 2008

Let $ y(t)=\int_{-\infty}^{\infty}2x(t)dt $

Then $ h(t) =2u(t) $

And $ H(s) = \int_{-\infty}^{\infty}h(t)e^{-st}dt $

$ =\int_{-\infty}^{\infty}2u(t)e^{-st}dt $

$ =\int_{0}^{\infty}2e^{-st}dt $

$ =(\frac{-2}{s}e^{-st})|_{0}^{\infty} $

$ =\frac{2}{s} $

Alumni Liaison

Ph.D. on Applied Mathematics in Aug 2007. Involved on applications of image super-resolution to electron microscopy

Francisco Blanco-Silva