HW 05: Difference between revisions

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|<math>=\delta(\omega_0-\omega)\,\!</math>
|<math>=\delta(\omega_0-\omega)\,\!</math>
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|<math>F[\cos {\omega_0 t}]\,\!</math>
|<math>=\int_{-\infty}^{\infty}\frac{e^{j\omega_0 t} + e^{-j\omega_0 t}}{2} e^{-j \omega t}dt</math>
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|<math>=\frac{1}{2}\int_{-\infty}^{\infty}\left (e^{j\omega_0 t} + e^{-j\omega_0 t}\right )2e^{-j \omega t} dt</math>
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|<math>=\frac{1}{2}\int_{-\infty}^{\infty} 2e^{j(\omega_0-\omega) t} + 2e^{-j(\omega_0+\omega) t} dt</math>
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|<math>=\int_{-\infty}^{\infty} e^{j(\omega_0-\omega) t} + e^{-j(\omega_0+\omega) t}</math>
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|<math>=\delta(\omega_0-\omega) + \delta(\omega_0+\omega)\,\!</math>
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Revision as of 16:40, 17 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
=δ(ω0−ω)
F[cos⁡ω0t] =∫−∞∞ejω0t+e−jω0t2e−jωtdt
=12∫−∞∞(ejω0t+e−jω0t)2e−jωtdt
=12∫−∞∞2ej(ω0−ω)t+2e−j(ω0+ω)tdt
=∫−∞∞ej(ω0−ω)t+e−j(ω0+ω)t
=δ(ω0−ω)+δ(ω0+ω)