v¡(t) CCT1 R₁ R₁ = CCT2 Li ooooo L2 5 L₁ R2 R Rf 1 OA1 + + OA2 R ip#, Up# in#, Vn# Ra Rd CCT3 OA3 Ro Love OA# Ro Vo# vo(t) S s² + 25wns +w2²/12 For CCT2, prove that the 2nd order high pass filter can be written as: damping ratio 5 natural frequency = Wn Derived expressions for K, the damping ratio, and natural frequency in terms of CCT parameters (L1, L2, R1, R2, R). T₂(s) = K-

v¡(t) CCT1 R₁ R₁ = CCT2 Li ooooo L2 5 L₁ R2 R Rf 1 OA1 + + OA2 R ip#, Up# in#, Vn# Ra Rd CCT3 OA3 Ro Love OA# Ro Vo# vo(t) S s² + 25wns +w2²/12 For CCT2, prove that the 2nd order high pass filter can be written as: damping ratio 5 natural frequency = Wn Derived expressions for K, the damping ratio, and natural frequency in terms of CCT parameters (L1, L2, R1, R2, R). T₂(s) = K-

Introductory Circuit Analysis (13th Edition)

13th Edition

ISBN:9780133923605

Author:Robert L. Boylestad

Publisher:Robert L. Boylestad

Chapter1: Introduction

Section: Chapter Questions

Problem 1P: Visit your local library (at school or home) and describe the extent to which it provides literature...

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