Lecture 16_17_v2

# Lecture 16_17_v2 - Lecture 16 17 RLC finding the natural...

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Lecture 16 + 17 RLC: finding the natural response different kinds of damping

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Parallel RLC circuit • KCL gave us a 2 nd order differential equation – Can reformulate in a general form – Subbing in an exponential gives a quadratic equation • Solve for roots • Question: how does behavior change as a function of ω 0 , α ? • 3 cases of interest ( 29 2 0 2 2 2 0 2 2 0 2 0 2 2 2 2 1 2 1 2 1 2 1 0 exp 1 , 2 1 2 1 0 ϖ α - ± - = - ± - = + + = + + = = = = + + = + + = LC RC RC s V s s LC RC s s st V LC RC V dt dV dt V d LC V dt dV RC dt V d + V - L C R I L I C I R
Case 1: over damped • If α > ω 0, then Has two real roots, specifically: – Note that τ 1> τ 1 • Solution takes the form: • Where initial conditions dictate that 2 2 0 2 2 1 2 0 2 1 1 1 τ ϖ α - = - - - = - = - + - = s s 2 0 2 - ± - = s + V - L C R I L I C I R ( 29 t s t s Be Ae t V 2 1 - - + = ( 29 ( 29 ( 29 ( 29 2 1 0 0 0 0 Bs As C I RC V dt dV B A V L + = - - = + =

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2 nd order RC also over damped
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## This note was uploaded on 11/21/2011 for the course ECE 2100 taught by Professor Kelley/seyler during the Spring '05 term at Cornell.

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Lecture 16_17_v2 - Lecture 16 17 RLC finding the natural...

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