ASN4 -Fourier Transform property: Difference between revisions

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(New page: Back to my home page '''Find '''<math>\mathcal{F}[cos(w_0t)g(t)]\!</math> Recall <math> w_0 = 2\pi f_0\!</math>, so <math>\mathcal{F}[cos(w_0t)g(t)] = \mathcal{F}[cos(...)
 
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[[Jodi Hodge| Back to my home page]]
[[Jodi Hodge| Back to my home page]]


'''Find '''<math>\mathcal{F}[cos(w_0t)g(t)]\!</math>
'''Find '''<math>\mathcal{F}[cos(2\pi f_0t)g(t)]\!</math>


Recall <math> w_0 = 2\pi f_0\!</math>, so
Recall <math> w_0 = 2\pi f_0\!</math>, so


<math>\mathcal{F}[cos(w_0t)g(t)] = \mathcal{F}[cos(2\pi f_0t)g(t)] = \int_{-\infty}^{\infty}cos(2\pi f_0t)g(t)e^{-j2\pi ft}dt\!</math>
Using Euler's cosine identity <math>\int_{-\infty}^{\infty}cos(2\pi f_0t)g(t)e^{-j2\pi ft}dt = \int_{-\infty}^{\infty} \frac{1}{2}[e^{j2\pi f_0t}+e^{-j2\pi f_0t}]g(t)e^{-j2\pi ft}dt\!</math>


Using Euler's cosine identity <math>\int_{-\infty}^{\infty}cos(2\pi f_0t)g(t)e^{-j2\pi ft}dt = \int_{-\infty}^{\infty} \frac{1}{2}[e^{j2\pi f_0t}+e^{-j2\pi f_0t}]g(t)e^{-j2\pi ft}dt\!</math>
Now <math> \mathcal{F}[cos(2\pi f_0t)g(t)]= \frac{1}{2}\int_{-\infty}^{\infty}e^{-j2\pi (f-f_0)t}g(t)dt \ + \ \frac{1}{2}\int_{-\infty}^{\infty}e^{-j2\pi (f+f_0)t}g(t)dt \!</math>


Now <math>\int_{-\infty}^{\infty} \frac{1}{2}[e^{j2\pi f_0t}+e^{-j2\pi f_0t}]g(t)e^{-j2\pi ft}dt = \frac{1}{2}\int_{-\infty}^{\infty}e^{-j2\pi (f-f_0)t}g(t)dt \ + \ \frac{1}{2}\int_{-\infty}^{\infty}e^{-j2\pi (f+f_0)t}g(t)dt = \frac{1}{2}G(f-f_0) \ + \ \frac{1}{2}G(f+f_0)\!</math><br><br>
So <math>\mathcal{F}[cos(2\pi f_0t)g(t)] = \frac{1}{2}[G(f-f_0)+ G(f+f_0)]\!</math>
So <math>\mathcal{F}[cos(w_0t)g(t)] = \frac{1}{2}[G(f-f_0)+ G(f+f_0)]\!</math><br><br>

Revision as of 23:43, 18 December 2009

Back to my home page

Find

Recall , so

Using Euler's cosine identity

Now

So