10/09 - Fourier Transform: Difference between revisions

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==Examples==
==Examples==
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|<math>\int_{-\infty}^{\infty}e^{j2\pi ft}e^{-j2\pi f\lambda}df</math>
|<math>=\left\langle e^{j2\pi ft}\mid e^{j2\pi ft}\right\rangle_f</math>
|<math>=\delta(t-\lambda)\,\!</math>
|-
|<math>\int_{-\infty}^{\infty}e^{j2\pi tf}e^{-j2\pi tf_0}dt</math>
|<math>=\left\langle e^{j2\pi tf}\mid e^{j2\pi tf_0}\right\rangle_t</math>
|<math>=\delta(f-f_0)\,\!</math>
|}

{| border="0" cellpadding="0" cellspacing="0"
{| border="0" cellpadding="0" cellspacing="0"
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===Sifting property of the delta function===
===Sifting property of the delta function===

{| border="0" cellpadding="0" cellspacing="0"
|-
|<math>\int_{-\infty}^{\infty}e^{j2\pi ft}e^{-j2\pi f\lambda}df</math>
|<math>=\left\langle e^{j2\pi ft}\mid e^{j2\pi ft}\right\rangle_f</math>
|<math>=\delta(t-\lambda)\,\!</math>
|-
|<math>\int_{-\infty}^{\infty}e^{j2\pi tf}e^{-j2\pi tf_0}dt</math>
|<math>=\left\langle e^{j2\pi tf}\mid e^{j2\pi tf_0}\right\rangle_t</math>
|<math>=\delta(f-f_0)\,\!</math>
|}

Revision as of 17:09, 17 November 2008

Assuming the function is perodic with the period T

Fourier Transform

Remember from 10/02 - Fourier Series

If we let

Remember

Definitions

Examples

Sifting property of the delta function