ASN4 fixing: Difference between revisions

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<math> (|s(t)|)^2 = \int_{- \infty}^{\infty}\int_{- \infty}^{\infty}S(f)e^{j 2 \pi f t} S(f)e^{-j 2 \pi f' t} df df^'</math>
<math> (|s(t)|)^2 = \int_{- \infty}^{\infty}\int_{- \infty}^{\infty}S(f)e^{j 2 \pi f t} S(f)e^{-j 2 \pi f' t} df df^'</math>
<math> s(t)e^{-j 2 \pi f t}e^{j 2 \pi f t} s(t)e^{-j 2 \pi f t}e^{-j 2 \pi f' t} df df^'</math>


and
and

Revision as of 23:10, 13 December 2009

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Parseval's Theorem

Parseval's Theorem says that ∫−∞∞(|s(t)|)2dt in time transforms to ∫−∞∞(|S(f)|)2df in frequency

Note that (|s(t)|)2=s(t).s*(t)

and also that

s(t)=F−1[S(f)]=∫−∞∞S(f)ej2πftdf

Therefore

(|s(t)|)2=∫−∞∞∫−∞∞S(f)ej2πftS(f)e−j2πf′tdfdf'

s(t)e−j2πftej2πfts(t)e−j2πfte−j2πf′tdfdf'

and

∫−∞∞(|s(t)|)2dt=∫−∞∞∫−∞∞∫−∞∞S(f)ej2πftS(f)e−j2πf′tdfdf'dt

Note that

The above equation of |s(t)| simplifies to then |s(t)|=∫−∞∞S(f)df=|S(f)|

Therefore,squaring the function and intergrating it in the time domain ∫−∞∞(|s(t)|)2dt is to do the same in the frequency domain ∫−∞∞(|S(f)|)2df