EET 300 Lecture Notes - Lecture 12: Inductor, Nodal Analysis, V Engine

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Transforms was to be able to use it to simplify difficult circuit analysis. In order to do so, we need to convert circuits into the s-domain. i(t) If the capacitor has an initial charge on it, then we can represent it in one of two ways. The same type of thing can be done with inductors with an initial flux: Once the circuit has been transformed into the s-domain, you no longer have to worry about whether a device is a resistor, capacitor, or an inductor. The difference in which they react in the time domain has been taken care of by their transforms. I n chapter 4 we fo und that: i( ) t i( Kvl (leaving out the s ( ) till the end for larity) c. Before converting back to the time domain we need to get the coefficient of to 1 . Ended up with the same result in both methods!

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