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| <math>\sum^{\infty}_{k=-\infty} a_{k}e^{jkw_{0}t} </math> || <math>2\pi\sum^{\infty}_{k=-\infty}a_{k}\delta(w-kw_{0})\,</math> || <math> a_k </math>
 
| <math>\sum^{\infty}_{k=-\infty} a_{k}e^{jkw_{0}t} </math> || <math>2\pi\sum^{\infty}_{k=-\infty}a_{k}\delta(w-kw_{0})\,</math> || <math> a_k </math>
 
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| {{Help:Section#Section_linking|Section linking}}|| {{:CT_Fourier Pairs 3_test}} || yz
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| {{:CT_Fourier_Pair_3_signal}} || {{:CT_Fourier_Pair_3_FT}} || yz
 
|- align="center"
 
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Revision as of 13:40, 15 October 2008

Signal Fourier transform Fourier series coefficients (if periodic)
$ \sum^{\infty}_{k=-\infty} a_{k}e^{jkw_{0}t} $ $ 2\pi\sum^{\infty}_{k=-\infty}a_{k}\delta(w-kw_{0})\, $ $ a_k $
CT Fourier Pair 3 signal CT Fourier Pair 3 FT yz

Alumni Liaison

Abstract algebra continues the conceptual developments of linear algebra, on an even grander scale.

Dr. Paul Garrett