ASN4 - Fourier Transform property: Parseval's Theorem: Difference between revisions
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Jodi.Hodge (talk | contribs) |
Jodi.Hodge (talk | contribs) |
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Note that <math> |e^{j 2 \pi f t}|= \sqrt{cos^2(2 \pi f t) + sin^2(2 \pi f t)}=1 </math> |
Note that <math> |e^{j 2 \pi f t}|= \sqrt{cos^2(2 \pi f t) + sin^2(2 \pi f t)}=1 </math> |
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So then <math>|s(t)|= \int_{- \infty}^{\infty}S(f) df</math> |
So then <math>|s(t)|= \int_{- \infty}^{\infty}S(f) df= |S(f)|</math> |
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Squareing the function and intergrating in the time main <math>\int_{- \infty}^{\infty} (|s(t)|)^2 dt</math> is to do the same in the frequency domain <math>\int_{- \infty}^{\infty} (|S(f)|)^2 df</math> |
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<math>Insert formula here</math> |
Revision as of 02:09, 30 November 2009
Parseval's Theorem
in time transforms to in frequency
The magnitude of is also the Inverse Fourier Transform of .
Note that
So then
Squareing the function and intergrating in the time main is to do the same in the frequency domain