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Physics 102: Lecture 7, Slide 1 RC Circuits Textbook Section 18.10-11 Physics 102: Lecture 7
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Physics 102: Lecture 7, Slide 2 Combine R+C Circuits Gives time dependence –Current is not constant I(t) –Charge is not constant q(t) Used for timing –Pacemaker –Intermittent windshield wipers Models nervous system include R, C –Sports Trivia: How soon after starting gun can you run w/o getting a False Start?
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Physics 102: Lecture 7, Slide 3 RC Circuits: Charging KVL: Just after S 1 is closed: ______ –Capacitor is uncharged (no time has –passed so charge hasn’t changed yet) Long time after: __________ –Capacitor is fully charged Intermediate (more complex) q(t) = q (1-e -t/RC ) I(t) = I 0 e -t/RC C R S1S1 S2S2 + + + I - - - The switches are originally open and the capacitor is uncharged. Then switch S 1 is closed. t q RC 2RC 0 qq
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Physics 102: Lecture 7, Slide 4 Capacitor “Rules of Thumb” Initially uncharged capacitor: –acts like a wire (short circuit) at t = 0 –acts like an open circuit (broken wire) as t Initially charged capacitor: –acts like a battery at t = 0
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Physics 102: Lecture 7, Slide 5 Time Constant Demo Which system will be brightest? Which lights will stay on longest? Which lights consumes more energy? 2 Each circuit has a 1 F capacitor charged to 100 Volts. When the switch is closed: 1 = 2RC = RC/2
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Physics 102: Lecture 7, Slide 6 Time Constant Demo Which system will be brightest? Which lights will stay on longest? Which lights consumes more energy? 2 Each circuit has a 1 F capacitor charged to 100 Volts. When the switch is closed: 1 = 2RC = RC/2 2 I=2V/R 1 Same U=1/2 CV 2
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Physics 102: Lecture 7, Slide 7 Preflight 7.1, 7.3 2R C R S2S2 Both switches are initially open, and the capacitor is uncharged. What is the current through the battery just after switch S 1 is closed? 1) I b = 02) I b = /(3R) 3) I b = /(2R)4) I b = /R S1S1 IbIb + - + + - - Both switches are initially open, and the capacitor is uncharged. What is the current through the battery after switch 1 has been closed a long time?long time 1) I b = 0 2) I b = V/(3R) 3) I b = V/(2R) 4) I b = V/R
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Physics 102: Lecture 7, Slide 8 ACT: RC Circuits Both switches are closed. What is the final charge on the capacitor after the switches have been closed a long time? 1) Q = 02) Q = C /3 3) Q = C /24) Q = C R 2R C S2S2 S1S1 IRIR + - + + - - + -
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Physics 102: Lecture 7, Slide 9 ACT: RC Circuits Both switches are closed. What is the final charge on the capacitor after the switches have been closed a long time? 1) Q = 02) Q = C / 3 3) Q = C /24) Q = C KVL (right loop): -Q/C+IR = 0 KVL (outside loop), - + I(2R) + IR = 0 I = /(3R) combine: -Q/C + /(3R) R = 0 Q = C ε / 3 R 2R C S2S2 S1S1 IRIR + - + + - - + -
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Physics 102: Lecture 7, Slide 10 Practice! Calculate current immediately after switch is closed: Calculate current after switch has been closed for 0.5 seconds: Calculate current after switch has been closed for a long time: Calculate charge on capacitor after switch has been closed for a long time: R C E S1S1 R=10 C=30 mF E =20 Volts -
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Practice! Calculate current immediately after switch is closed: Calculate current after switch has been closed for 0.5 seconds: Calculate current after switch has been closed for a long time: Calculate charge on capacitor after switch has been closed for a long time: R C E S1S1 R=10 C=30 mF E =20 Volts - + I 0 R + q 0 /C = 0 I + + + - - - - + I 0 R + 0 = 0 I 0 = /R After a long time current through capacitor is zero! - + IR + q ∞ /C = 0 - + 0 + q ∞ /C = 0 q ∞ = C
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Physics 102: Lecture 7, Slide 12 Charging: Intermediate Times Calculate the charge on the capacitor 3 10 -3 seconds after switch 1 is closed. q(t) = q (1-e -t/RC ) C R1R1 S2S2 S1S1 IbIb + - + + - - R 1 = 20 R 2 = 40 ε = 50 Volts C = 100 F R2R2
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Physics 102: Lecture 7, Slide 13 Charging: Intermediate Times C R1R1 S2S2 S1S1 IbIb + - + + - - Calculate the charge on the capacitor 3 10 -3 seconds after switch 1 is closed. q(t) = q (1-e -t/R 2 C ) = q (1-e - 3 10 -3 /(40 100 10 -6) ) ) = q (0.53) Recall q = ε C = (50)(100x10 -6 ) (0.53) = 2.7 x10 -3 Coulombs R 1 = 20 R 2 = 40 ε = 50 Volts C = 100 F R2R2
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Physics 102: Lecture 7, Slide 14 RC Circuits: Discharging KVL: ____________ Just after…: ________ –Capacitor is still fully charged Long time after: ____________ Intermediate (more complex) –q(t) = q 0 e -t/RC –I c (t) = I 0 e -t/RC C R S1S1 - + + I - + - S2S2 q RC2RC t
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Physics 102: Lecture 7, Slide 15 RC Circuits: Discharging KVL: - q(t) / C - I(t) R = 0 Just after…: q=q 0 –Capacitor is still fully charged –-q 0 / C - I 0 R = 0 I 0 = q 0 /(RC) Long time after: I c =0 –Capacitor is discharged –-q / C = 0 q = 0 Intermediate (more complex) –q(t) = q 0 e -t/RC –I c (t) = I 0 e -t/RC C R S1S1 - + + I - + - S2S2 q RC2RC t
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Physics 102: Lecture 7, Slide 16 Preflight 7.5 After switch 1 has been closed for a long time, it is opened and switch 2 is closed. What is the current through the right resistor just after switch 2 is closed? 1) I R = 02) I R = /(3R) 3) I R = /(2R)4) I R = /R 2R C R S2S2 S1S1 IRIR + - + + - - + -
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Physics 102: Lecture 7, Slide 17 Preflight 7.5 After switch 1 has been closed for a long time, it is opened and switch 2 is closed. What is the current through the right resistor just after switch 2 is closed? 1) I R = 02) I R = /(3R) 3) I R = /(2R)4) I R = /R KVL: -q 0 /C+IR = 0 Recall q is charge on capacitor after charging: q 0 = C (since charged w/ switch 2 open!) - + IR = 0 I = /R 2R C R S2S2 S1S1 IRIR + - + + - - + -
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Physics 102: Lecture 7, Slide 18 ACT: RC Challenge 1) 0.368 q 0 2) 0.632 q 0 3) 0.135 q 0 4) 0.865 q 0 2R C E R S1S1 E = 24 Volts R = 4 C = 15 mF After being closed for a long time, the switch is opened. What is the charge Q on the capacitor 0.06 seconds after the switch is opened?
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Physics 102: Lecture 7, Slide 19 ACT: RC Challenge 1) 0.368 q 0 2) 0.632 q 0 3) 0.135 q 0 4) 0.865 q 0 2R C E R S1S1 E = 24 Volts R = 4 C = 15 mF After being closed for a long time, the switch is opened. What is the charge Q on the capacitor 0.06 seconds after the switch is opened? q(t) = q 0 e -t/RC = q 0 (e - 0.06 /(4 (15 10 -3 )) ) = q 0 (0.368)
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Physics 102: Lecture 7, Slide 20 RC Summary ChargingDischarging q(t) = q (1-e -t/RC )q(t) = q 0 e -t/RC V(t) = V (1-e -t/RC )V(t) = V 0 e -t/RC I(t) = I 0 e -t/RC Short term: Charge doesn’t change (often zero or max) Long term: Current through capacitor is zero. Time Constant = RC Large means long time to charge/discharge
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Physics 102: Lecture 7, Slide 21 See you next lecture! Read Textbook Sections 19.1-4
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