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>
<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)=F1[S(f)]=S(f)ej2πftdf

Therefore

(|s(t)|)2=S(f)ej2πftS(f)ej2πftdfdf'

s(t)ej2πftej2πfts(t)ej2πftej2πftdfdf'

and

(|s(t)|)2dt=S(f)ej2πftS(f)ej2πftdfdf'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