ASN4 -Fourier Transform property: Difference between revisions

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<math> = \int_{-\infty}^{\infty} [\frac{1}{2}e^{j2\pi f_0t}+\frac{1}{2}e^{-j2\pi f_0t}]g(t)e^{-j2\pi ft}dt\!</math>
<math> = \int_{-\infty}^{\infty} [\frac{1}{2}e^{j2\pi f_0t}+\frac{1}{2}e^{-j2\pi f_0t}]g(t)e^{-j2\pi ft}dt\!</math>


Distribting to both terms in side the brackets
Distribting to both terms in side the brackets


<math> = \int_{-\infty}^{\infty} \frac{1}{2}e^{j2\pi f_0t}e^{-j2\pi ft} dt + \int_{-\infty}^{\infty}\frac{1}{2}e^{-j2\pi f_0t}g(t)e^{-j2\pi ft}dt\!</math>
<math> = \int_{-\infty}^{\infty} \frac{1}{2}e^{j2\pi f_0t}e^{-j2\pi ft} dt + \int_{-\infty}^{\infty}\frac{1}{2}e^{-j2\pi f_0t}g(t)e^{-j2\pi ft}dt\!</math>

Latest revision as of 11:37, 19 December 2009

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Find the Fourier transform of cos(2πf0t)g(t)


ℱ[cos(2πf0t)g(t)]

Applying the forward Fourier transform

=∫−∞∞cos(2πf0t)g(t)e−j2πftdt

Applying Euler's cosine identity

=∫−∞∞[12ej2πf0t+12e−j2πf0t]g(t)e−j2πftdt

Distribting to both terms in side the brackets

=∫−∞∞12ej2πf0te−j2πftdt+∫−∞∞12e−j2πf0tg(t)e−j2πftdt

Combining exponential terms

=∫−∞∞12e−j2π(f−f0)tg(t)dt+∫−∞∞12e−j2π(f+f0)tg(t)dt

Note that there are forward Fourier Transform expressions in the above equation. With substitution the result is

ℱ[cos(2πf0t)g(t)]=12G(f−f0)+12[G(f+f0)