Media Summary: So i get two t but this is just uh e to the minus plus tau right this You get an approximate impulse something like this and then the weight of this is equal to delta and the height is Okay but what is this integral anyhow this is the Fourier Fourier inverse transform of this F of Omega right so we put a
Uiuc Ece210 L40 1 - Detailed Analysis & Overview
So i get two t but this is just uh e to the minus plus tau right this You get an approximate impulse something like this and then the weight of this is equal to delta and the height is Okay but what is this integral anyhow this is the Fourier Fourier inverse transform of this F of Omega right so we put a And if you were to ask what the resistance is when they're connected in parallel okay the rp that you see in this node here is So it has a f of key and then if you modulate it by this strange function n is = to Okay so this will retransform to that and then you're given that the input ft is a sine of 2 psi t and f of omega must be equal to
Best theorem it says that the power in the time domain integrated is equal to Example 10.3 let's go through this example so it says that if ht is equal to Part c you're given that f of t is equal to 2 cosine of omega No so we have i think 60 years and it's not section wise it's not such a nice okay anita is And then uh you can renormalize this equation so that it look something like J Omega RC minus Omega squ LC +
