HW 05: Difference between revisions

From Class Wiki
Jump to navigation Jump to search
Fonggr (talk | contribs)
Fonggr (talk | contribs)
No edit summary
 
(7 intermediate revisions by the same user not shown)
Line 1: Line 1:
Find the following Fourier Transforms
Find the following Fourier Transforms
*<math>F[e^{j \omega_0 t}]</math>
*<math>F\left[e^{j \omega_0 t}\right]</math>
*<math>F[\cos {\omega_0 t}]\,\!</math>
*<math>F\left[\cos {\omega_0 t}\right]\,\!</math>
*<math>F[\sum_{-\infty}^{\infty}\alpha_n e^{j2\pi nt/T}]</math>
*<math>F\left[\sum_{-\infty}^{\infty}\alpha_n e^{j2\pi nt/T}\right]</math>
*<math>F[\sin{\omega_0 t}]\,\!</math>
*<math>F\left[\sin{\omega_0 t}\right]\,\!</math>


==Solutions==
==Solutions==
{| border="0" cellpadding="0" cellspacing="0"
{| border="0" cellpadding="0" cellspacing="0"
|-
|-
|<math>F[e^{j \omega_0 t}]</math>
|<math>F\left[e^{j \omega_0 t}\right]</math>
|<math>=\int_{-\infty}^{\infty} e^{j \omega_0 t} e^{-j \omega t}dt</math>
|<math>=\int_{-\infty}^{\infty} e^{j \omega_0 t} e^{-j \omega t}dt</math>
|-
|-
Line 20: Line 20:
|<math>=2\pi \delta(\omega_0-\omega)\,\!</math>
|<math>=2\pi \delta(\omega_0-\omega)\,\!</math>
|-
|-
|<math>F[\cos {\omega_0 t}]\,\!</math>
|<math>F\left[\cos {\omega_0 t}\right]\,\!</math>
|<math>=\int_{-\infty}^{\infty}\frac{e^{j\omega_0 t} + e^{-j\omega_0 t}}{2} e^{-j \omega t}dt</math>
|<math>=\int_{-\infty}^{\infty}\frac{e^{j\omega_0 t} + e^{-j\omega_0 t}}{2} e^{-j \omega t}dt</math>
|-
|-
|
|
|<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>
|<math>=\frac{1}{2}\int_{-\infty}^{\infty}\left (e^{j\omega_0 t} + e^{-j\omega_0 t}\right )e^{-j \omega t} dt</math>
|-
|-
|
|
|<math>=\frac{1}{2}\int_{-\infty}^{\infty} \left [2e^{j(\omega_0-\omega) t} + 2e^{-j(\omega_0+\omega) t}\right ] dt</math>
|<math>=\frac{1}{2}\int_{-\infty}^{\infty} \left [e^{j(\omega_0-\omega) t} + e^{-j(\omega_0+\omega) t}\right ] dt</math>
|-
|-
|
|
|<math>=2\pi\left [ \frac{1}{2\pi}\int_{-\infty}^{\infty} \left (e^{j(\omega_0-\omega) t} + e^{-j(\omega_0+\omega) t}\right )\,dt\right]</math>
|<math>=\pi\left [ \frac{1}{2\pi}\int_{-\infty}^{\infty} \left (e^{j(\omega_0-\omega) t} + e^{-j(\omega_0+\omega) t}\right )\,dt\right]</math>
|-
|-
|
|
|<math>=2\pi\delta(\omega_0-\omega) + 2\pi\delta(\omega_0+\omega)\,\!</math>
|<math>=\pi\delta(\omega_0-\omega) + \pi\delta(\omega_0+\omega)\,\!</math>
|-
|-
|<math>F[\sin{\omega_0 t}]\,\!</math>
|<math>F\left[\sin{\omega_0 t}\right]\,\!</math>
|<math>=\int_{-\infty}^{\infty}\frac{e^{j\omega_0 t} - e^{-j\omega_0 t}}{2j} e^{-j \omega t}dt</math>
|<math>=\int_{-\infty}^{\infty}\frac{e^{j\omega_0 t} - e^{-j\omega_0 t}}{2j} e^{-j \omega t}dt</math>
|-
|
|<math>=\frac{1}{2j}\int_{-\infty}^{\infty}\left (e^{j\omega_0 t} - e^{-j\omega_0 t}\right )e^{-j \omega t} dt</math>
|-
|
|<math>=\frac{1}{2j}\int_{-\infty}^{\infty} \left (e^{j(\omega_0-\omega) t} - e^{-j(\omega_0+\omega) t}\right ) dt</math>
|-
|
|<math>=\frac{\pi}{j}\left [ \frac{1}{2\pi}\int_{-\infty}^{\infty} \left (e^{j(\omega_0-\omega) t} - e^{-j(\omega_0+\omega) t}\right )\,dt\right]</math>
|-
|
|<math>=-j\pi\delta(\omega_0-\omega) + j\pi\delta(\omega_0+\omega)\,\!</math>
|-
|<math>F\left[\sum_{-\infty}^{\infty}\alpha_n e^{j2\pi nt/T}\right]</math>
|<math>=\int_{-\infty}^{\infty} \left (\sum_{-\infty}^{\infty}\alpha_n e^{j2\pi nt/T} \right )e^{-j \omega t}dt</math>
|-
|
|<math>=\sum_{-\infty}^{\infty}\alpha_n \left (\int_{-\infty}^{\infty} e^{j2\pi nt/T} e^{-j2\pi ft}dt\right )</math>
|-
|
|<math>=\sum_{-\infty}^{\infty}\alpha_n \left (\int_{-\infty}^{\infty} e^{j2\pi t (\frac{n}{T}-f)} dt\right )</math>
|-
|
|<math>=\sum_{-\infty}^{\infty}\alpha_n \delta\left(\frac{n}{T}-f\right) </math>
|}
|}

Latest revision as of 21:27, 23 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)e−jωtdt
=12∫−∞∞[ej(ω0−ω)t+e−j(ω0+ω)t]dt
=π[12π∫−∞∞(ej(ω0−ω)t+e−j(ω0+ω)t)dt]
=πδ(ω0−ω)+πδ(ω0+ω)
F[sin⁡ω0t] =∫−∞∞ejω0t−e−jω0t2je−jωtdt
=12j∫−∞∞(ejω0t−e−jω0t)e−jωtdt
=12j∫−∞∞(ej(ω0−ω)t−e−j(ω0+ω)t)dt
=πj[12π∫−∞∞(ej(ω0−ω)t−e−j(ω0+ω)t)dt]
=−jπδ(ω0−ω)+jπδ(ω0+ω)
F[∑−∞∞αnej2πnt/T] =∫−∞∞(∑−∞∞αnej2πnt/T)e−jωtdt
=∑−∞∞αn(∫−∞∞ej2πnt/Te−j2πftdt)
=∑−∞∞αn(∫−∞∞ej2πt(nT−f)dt)
=∑−∞∞αnδ(nT−f)