September 2008
Beginner
834 pages
37h 13m
English
We arrived at the Fourier transform of δ(t) against the background of time-domain compression of waveforms in the last section. Further, by applying duality principle on this Fourier transform, we derived the Fourier transform for v(t) = 1. Then, we tried to obtain the Fourier transform by applying analysis integral on v(t) = 1 and ended up with an improper integral. We remembered the theorem of uniqueness of Fourier transforms and assigned 2πτ(jω) to this integral, since we had seen by other means that this is the Fourier transform of v(t) = 1. This integral is
We observe that the variable of integration ...
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