3. You have seen how Kirchhoff's laws were used in your lectures to obtain a 2na order differential equation where we solved for the current. This time we wll use an even simpler concept: principle of conservation of energy to derive the 2nd order differential equation where we will solve for the charge. Take a look at the circuit below. :2F In the circuit above, we have a capacitor with capacitance 2 F, an inductor of inductance 5 H and a resistor of 3N (c) Solve the differential equation for initial charge to be Qo with a initial current of -0.3Q0/s.

3. You have seen how Kirchhoff's laws were used in your lectures to obtain a 2na order differential equation where we solved for the current. This time we wll use an even simpler concept: principle of conservation of energy to derive the 2nd order differential equation where we will solve for the charge. Take a look at the circuit below. :2F In the circuit above, we have a capacitor with capacitance 2 F, an inductor of inductance 5 H and a resistor of 3N (c) Solve the differential equation for initial charge to be Qo with a initial current of -0.3Q0/s.

Physics for Scientists and Engineers: Foundations and Connections

1st Edition

ISBN:9781133939146

Author:Katz, Debora M.

Publisher:Katz, Debora M.

Chapter32: Faraday’s Law Of Induction

Section: Chapter Questions

Problem 76PQ

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