Lect07 handout

795 views

Published on

Published in: Technology, Business
0 Comments
2 Likes
Statistics
Notes
  • Be the first to comment

No Downloads
Views
Total views
795
On SlideShare
0
From Embeds
0
Number of Embeds
29
Actions
Shares
0
Downloads
17
Comments
0
Likes
2
Embeds 0
No embeds

No notes for slide
  • 1
  • Initial current through battery. Final current; final voltage across C.
  • Initial current through battery. Final current; final voltage across C.
  • Initial current through battery. Final current; final voltage across C.
  • Followup…what is current a long time later? What is charge on capacitor a long time later?
  • Lect07 handout

    1. 1. RC Circuits Physics 102: Lecture 7
    2. 2. Recall …. <ul><li>First we covered circuits with batteries and capacitors </li></ul><ul><ul><li>series, parallel </li></ul></ul><ul><li>Then we covered circuits with batteries and resistors </li></ul><ul><ul><li>series, parallel </li></ul></ul><ul><ul><li>Kirchhoff’s Loop and Junction Relations </li></ul></ul><ul><li>Today: circuits with batteries, resistors, and capacitors </li></ul>
    3. 3. RC Circuits <ul><li>RC Circuits </li></ul><ul><li>Charging Capacitors </li></ul><ul><li>Discharging Capacitors </li></ul><ul><li>Intermediate Behavior </li></ul>
    4. 4. RC Circuits <ul><li>Circuits that have both resistors and capacitors : </li></ul><ul><li>With resistance in the circuits, capacitors do not charge and discharge instantaneously – it takes time (even if only fractions of a second). </li></ul>R K C S + + + R Na R Cl ε K ε Na ε Cl
    5. 5. Capacitors <ul><li>Charge (and therefore voltage) on Capacitors cannot change instantly: remember V C = Q/C </li></ul><ul><li>Short term behavior of Capacitor: </li></ul><ul><ul><li>If the capacitor starts with no charge, it has no potential difference across it and acts as a wire </li></ul></ul><ul><ul><li>If the capacitor starts with charge, it has a potential difference across it and acts as a battery. </li></ul></ul><ul><li>Long term behavior of Capacitor: Current through a Capacitor eventually goes to zero. </li></ul><ul><ul><li>If the capacitor is charging, when fully charged no current flows and capacitor acts as an open circuit </li></ul></ul><ul><ul><li>If capacitor is discharging, potential difference goes to zero and no current flows </li></ul></ul>
    6. 6. Charging Capacitors <ul><li>Capacitor is initially uncharged and switch is open. Switch is then closed. What is current I 0 in circuit immediately thereafter? </li></ul><ul><li>What is current I  in circuit a long time later? </li></ul> R C S
    7. 7. Charging Capacitors: t=0 <ul><li>Capacitor is initially uncharged and switch is open. Switch is then closed. What is current I 0 in circuit immediately thereafter? </li></ul><ul><ul><li>Capacitor initially uncharged </li></ul></ul><ul><ul><li>Therefore V C is initially 0 </li></ul></ul><ul><ul><li>Therefore C behaves as a wire (short circuit) </li></ul></ul><ul><ul><li>KLR:  – I 0 R = 0 </li></ul></ul><ul><ul><ul><li>I 0 =  /R </li></ul></ul></ul> R C S R 
    8. 8. Charging Capacitors: t>0 <ul><ul><li>I 0 =  /R </li></ul></ul><ul><ul><li>Positive charge flows </li></ul></ul><ul><ul><ul><li>Onto bottom plate (+Q) </li></ul></ul></ul><ul><ul><ul><li>Away from top plate (-Q) </li></ul></ul></ul><ul><ul><ul><li>As charge builds up, V C rises (V C =Q/C) </li></ul></ul></ul><ul><ul><ul><li>Loop:  – V C – I R = 0 </li></ul></ul></ul><ul><ul><ul><ul><li>I = (  -V C )/R </li></ul></ul></ul></ul><ul><ul><ul><ul><li>Therefore I falls as Q rises </li></ul></ul></ul></ul><ul><ul><li>When t is very large (  ) </li></ul></ul><ul><ul><ul><li>I  = 0: no current flow into/out of capacitor for t large </li></ul></ul></ul><ul><ul><ul><li>V C =  </li></ul></ul></ul> R C + - Demo R 
    9. 9. ACT/Preflight 7.1 <ul><li>Both switches are initially open, and the capacitor is uncharged. What is the current through the battery just after switch S 1 is closed? </li></ul>2R C  R S 2 1) I b = 0 2) I b = E /(3R) 3) I b = E /(2R) 4) I b = E /R S 1 I b + - + + - -
    10. 10. ACT/Preflight 7.3 <ul><li>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 ? </li></ul>1) I b = 0 2) I b = E /(3R) 3) I b = E /(2R) 4) I b = E /R 2R C  R S 2 S 1 I b + - + + - -
    11. 11. Discharging Capacitors <ul><li>Capacitor is initially charged (Q) and switch is open. Switch is then closed. What is current I 0 in circuit immediately thereafter? </li></ul><ul><li>What is current I  in circuit a long time later? </li></ul>R C S
    12. 12. Discharging Capacitors <ul><li>Capacitor is initially charged (Q) and switch is open. Switch is then closed. What is current I 0 in circuit immediately thereafter? </li></ul><ul><ul><li>KLR: Q/C – I 0 R = 0 </li></ul></ul><ul><ul><li>So, I 0 = Q/RC </li></ul></ul><ul><li>What is current I  in circuit a long time later? </li></ul><ul><ul><li>I  = 0 </li></ul></ul>R C + - Demo
    13. 13. ACT/Preflight 7.5 <ul><li>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? </li></ul>1) I R = 0 2) I R =  /(3R) 3) I R =  /(2R) 4) I R =  /R 2R C  R S 2 S 1 I R + - + + - - + -
    14. 14. ACT: RC Circuits <ul><li>Both switches are closed. What is the final charge on the capacitor after the switches have been closed a long time? </li></ul>1) Q = 0 2) Q = C E /3 3) Q = C E /2 4) Q = C E R 2R C  S 2 S 1 I R + - + + - - + -
    15. 15. RC Circuits: Charging <ul><li>Loop:  – I(t)R – q(t) / C = 0 </li></ul><ul><li>Just after…: q =q 0 </li></ul><ul><ul><li>Capacitor is uncharged </li></ul></ul><ul><ul><li> – I 0 R = 0  I 0 =  / R </li></ul></ul><ul><li>Long time after: I c = 0 </li></ul><ul><ul><li>Capacitor is fully charged </li></ul></ul><ul><ul><li> – q  /C =0  q  =  C </li></ul></ul><ul><li>Intermediate (more complex) </li></ul><ul><ul><li>q(t) = q  (1-e -t/RC ) </li></ul></ul><ul><ul><li>I(t) = I 0 e -t/RC </li></ul></ul>C  R S 1 S 2 + + + I - - - The switches are originally open and the capacitor is uncharged. Then switch S 1 is closed. t q RC 2RC 0 q 
    16. 16. RC Circuits: Discharging <ul><li>Loop: q(t) / C + I(t) R = 0 </li></ul><ul><li>Just after…: q=q 0 </li></ul><ul><ul><li>Capacitor is still fully charged </li></ul></ul><ul><ul><li>q 0 / C + I 0 R = 0  I 0 = –q 0 / (RC) </li></ul></ul><ul><li>Long time after: I c =0 </li></ul><ul><ul><li>Capacitor is discharged (like a wire) </li></ul></ul><ul><ul><li>q  / C = 0  q  = 0 </li></ul></ul><ul><li>Intermediate (more complex) </li></ul><ul><ul><li>q(t) = q 0 e -t/RC </li></ul></ul><ul><ul><li>I c (t) = I 0 e -t/RC </li></ul></ul>C  R S 1 - + + I - + - S 2 q RC 2RC t
    17. 17. What is the time constant? <ul><li>The time constant  = RC . </li></ul><ul><li>Given a capacitor starting with no charge, the time constant is the amount of time an RC circuit takes to charge a capacitor to about 63.2% of its final value. </li></ul><ul><li>The time constant is the amount of time an RC circuit takes to discharge a capacitor by about 63.2% of its original value. </li></ul>
    18. 18. Time Constant Demo <ul><li>Which system will be brightest? </li></ul><ul><li>Which lights will stay on longest? </li></ul><ul><li>Which lights consumes more energy? </li></ul>Each circuit has a 1 F capacitor charged to 100 Volts. When the switch is closed: 1 Example 2
    19. 19. Summary of Concepts <ul><li>Charge (and therefore voltage) on Capacitors cannot change instantly: remember V C = Q/C </li></ul><ul><li>Short term behavior of Capacitor: </li></ul><ul><ul><li>If the capacitor starts with no charge, it has no potential difference across it and acts as a wire </li></ul></ul><ul><ul><li>If the capacitor starts with charge, it has a potential difference across it and acts as a battery. </li></ul></ul><ul><li>Long term behavior of Capacitor: Current through a Capacitor eventually goes to zero. </li></ul><ul><ul><li>If the capacitor is charging, when fully charged no current flows and capacitor acts as an open circuit. </li></ul></ul><ul><ul><li>If capacitor is discharging, potential difference goes to zero and no current flows. </li></ul></ul><ul><li>Intermediate behavior: Charge and current exponentially approach their long-term values  = RC </li></ul>
    20. 20. 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: Example E – I 0 R – q 0 /C = 0 + + + - - - E – I 0 R – 0 = 0 I 0 = E /R After a long time current through capacitor is zero! E – IR – q ∞ /C = 0 E – 0 – q ∞ /C = 0 q ∞ = E C R C ε S 1 R=10  C=30 mF ε =20 Volts I
    21. 21. ACT: RC Challenge <ul><li>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? </li></ul>1) 0.368 q 0 2) 0.632 q 0 3) 0.135 q 0 4) 0.865 q 0 R C ε 2R S 1 ε = 24 Volts R = 2  C = 15 mF
    22. 22. Charging: Intermediate Times  Calculate the charge on the capacitor 3  10 -3 seconds after switch 1 is closed. <ul><ul><li>q(t) = q  (1-e -t/RC ) </li></ul></ul>= q  (1-e - 3  10 -3 /(20  100  10 -6) ) ) = q  (0.78) Recall q  =  C = (50)(100x10 -6 ) (0.78) = 3.9 x10 -3 Coulombs R = 10  V = 50 Volts C = 100  F Example 2R C R S 2 S 1 I b + - + + - -
    23. 23. RC Summary Charging Discharging 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 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

    ×