HW 05: Difference between revisions

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|<math>=2\pi\delta(\omega_0-\omega) - 2\pi\delta(\omega_0+\omega)\,\!</math>
|<math>=2\pi\delta(\omega_0-\omega) - 2\pi\delta(\omega_0+\omega)\,\!</math>
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|<math>F[\sum_{-\infty}^{\infty}\alpha_n e^{j2\pi nt/T}]</math>
|<math>=\int_{-\infty}^{\infty} \left (\sum_{-\infty}^{\infty}\alpha_n e^{j2\pi nt/T} \right )e^{-j \omega t}dt</math>
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|<math>=\sum_{-\infty}^{\infty}\alpha_n \left (\int_{-\infty}^{\infty} e^{j2\pi nt/T} e^{-j2\pi ft}dt\right )</math>
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||<math>=\sum_{-\infty}^{\infty}\alpha_n \left (\int_{-\infty}^{\infty} e^{j2\pi t (\frac{n}{T}-f)} dt\right )</math>
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Revision as of 00:43, 18 November 2008

Find the following Fourier Transforms

  • F[ejω0t]
  • F[cos⁡ω0t]
  • F[∑−∞∞αnej2πnt/T]
  • F[sin⁡ω0t]

Solutions

F[ejω0t] =∫−∞∞ejω0te−jωtdt
=∫−∞∞ej(ω0−ω)tdt
=2π[12π∫−∞∞ej(ω0−ω)tdt]
=2πδ(ω0−ω)
F[cos⁡ω0t] =∫−∞∞ejω0t+e−jω0t2e−jωtdt
=12∫−∞∞(ejω0t+e−jω0t)2e−jωtdt
=12∫−∞∞[2ej(ω0−ω)t+2e−j(ω0+ω)t]dt
=2π[12π∫−∞∞(ej(ω0−ω)t+e−j(ω0+ω)t)dt]
=2πδ(ω0−ω)+2πδ(ω0+ω)
F[sin⁡ω0t] =∫−∞∞ejω0t−e−jω0t2je−jωtdt
=12j∫−∞∞(ejω0t−e−jω0t)2je−jωtdt
=∫−∞∞(ej(ω0−ω)t−e−j(ω0+ω)t)dt
=2π[12π∫−∞∞(ej(ω0−ω)t−e−j(ω0+ω)t)dt]
=2πδ(ω0−ω)−2πδ(ω0+ω)
F[∑−∞∞αnej2πnt/T] =∫−∞∞(∑−∞∞αnej2πnt/T)e−jωtdt
=∑−∞∞αn(∫−∞∞ej2πnt/Te−j2πftdt)
=∑−∞∞αn(∫−∞∞ej2πt(nT−f)dt)
  • Think something went wrong here.