BLM1612 Circuit Theory Basic RL and RC Circuits 1 Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Capacitors and Inductors C→L v→i i →v The Source-Free RL Circuit Applying KVL: di R + i =0 dt L We can solve for the natural response if we know the initial condition i(0)=I0: i(t)=I0e-Rt/L for t>0 3 Example 8.2: RL with a Switch Show that the voltage v(t) will be -12.99 volts at t=200 ms. 4 The Exponential Response The time constant τ=L/R determines the rate of decay. i(t) = I0e −t /τ 5 The Source-Free RC Circuit Applying KCL: dv 1 + v =0 dt RC We can solve for the natural response if we know the initial condition v(0)=V0 v(t)=V0e-t/RC for t>0 6 RC Natural Response The time constant is τ=RC 7 Example 8.3: The Source Free RC Circuit Show that the voltage v(t) is 321 mV at t=200 µs. 8 General RL Circuits The time constant of a single-inductor circuit will be τ=L/Req where Req is the resistance seen by the inductor. Example: Req=R3+R4+R1R2 / (R1+R2) 9 General RC Circuits The time constant of a single-capacitor circuit will be τ=ReqC where Req is the resistance seen by the capacitor. Example 8.5: Req=R2+R1R3 / (R1+R3) Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required 10for reproduction or display. 1st Order Response Observations The voltage on a capacitor or the current through a inductor is the same prior to and after a switch at t=0. Resistor voltage (or current) prior to the switch v(0-) can be different from the voltage after the switch v(0+). All voltages and currents in an RC or RL circuit follow the same natural response e-t/τ. 11 Example 8.4: L and R Current Find i1(t) and iL(t) for t>0. Answer: τ=20 µs; i1=-0.24e-t/τ,iL=0.36e-t/τ for t>0 12 The Unit Step Function The unit-step function u(t) is a convenient notation to respresent change: 13 Switches and Steps The unit step models a double-throw switch. A single-throw switch is open circuit for t<0, not short circuit. 14 Modeling Pulses using u(t) Rectangular pulse Pulsed sinewave : 15 Driven RL Circuits The two circuits shown both have i(t)=0 for t<0 and are also the same for t>0. We now have to find both the natural response and and the forced response due to the source V0 – i=in+if – in=Ae-Rt/L – if=V0/R 16 Driven RL Circuits The total response is the combination of the transient/natural response and the forced response: V0 −Rt / L i(t) = (1 − e u(t) ) R 17 Driven RL Circuits V0 −Rt / L i(t) = (1 − e u(t) ) R 18 Example 8.7 For the circuit , find i(t) for t=∞, 3−, 3+, and 100 µs after the source changes value. Example 8.8: RL Circuit with Step Show that i(t)=25+25(1-e-t/2)u(t) A 20 Example 8.9: Voltage Pulse 21 Example 8.10: Driven RC Circuits (part 1 of 2) vC=20 + 80e-t/1.2 V and i=0.1 + 0.4e−t/1.2 A 22 Example 8.10: Driven RC Circuits (part 2 of 2) vC=20 + 80e-t/1.2 V i=0.1 + 0.4e−t/1.2 A 23 Chapter 8 Summary