Physics 212 Lecture 11, Slide 1 Physics 212 Lecture 11 RC Circuits Change in schedule Exam 2 will be...
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Transcript of Physics 212 Lecture 11, Slide 1 Physics 212 Lecture 11 RC Circuits Change in schedule Exam 2 will be...
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 11
Physics 212Physics 212Lecture 11Lecture 11
RC CircuitsRC Circuits
Change in scheduleChange in scheduleExam 2 will be on Thursday, July 12 from 8 – 9:30 AM.Exam 2 will be on Thursday, July 12 from 8 – 9:30 AM.
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 22
RC Circuit Charging
• Kirchoff’s Voltage Rule
• Initially (q = q0 = 0)
• Long Term (Ic =0)
RVbattery
Ca
bbattery
q-V + +IR = 0
C
00 0batteryV I R
battery0
VI =
R
0 0battery
qV R
C
batteryq CV
In general:
0battery
q dqV R
C dt
/( ) (1 )t RCq t q e /
0( ) t RCI t I e
11
a
RVbattery
C
b
• Capacitor uncharged, switch is moved to position “a”
II
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 3313
Checkpoint 1aCheckpoint 1a
Checkpoint 1bCheckpoint 1b&&
Close S1, Close S1, VV11 = voltage across C immediately after = voltage across C immediately afterVV22 = voltage across C a long time after = voltage across C a long time after
A)A) VV11 = V V = V V22 = V= VB) VB) V11 = 0 V = 0 V22 = V= VC) VC) V11 = 0 V = 0 V22 = 0= 0D) VD) V11 = V V = V V22 = 0= 0
Immediately after Immediately after the switch Sthe switch S11 is is closed:closed:
Q = 0Q = 0 VV11 = 0 = 0V = Q/CV = Q/C
After the switch SAfter the switch S11 has has been closed for a long been closed for a long timetime
I = 0I = 0 VV22 = V = VVVRR = 0 = 0
A circuit is wired up as shown below. The capacitor is initially uncharged and switches S1 and S2 are initially open.
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 44
V 2RC
R
S1 S2
Close SClose S11 at t=0 at t=0(leave S(leave S22 open) open)
For t For t
V C
R
I=0
VVCC = V = V
At t = 0At t = 0
V C
R
I
VVCC = Q/C = Q/C = 0= 0
15
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 55
RC Circuit (Discharging)
• Kirchoff’s Voltage Rule
• Initially (q=q0)
• Long Term (Ic =0)
RVbattery
Ca
b 0q
IRC
00 0
qI R
C
00
qI
RC
0 0q
RC
0q
In general:
0q dq
RC dt
/0( ) t RCq t q e
/0( ) t RCdq qI t e
dt RC
V
19
• Capacitor has q0 = CV, switch is moved to position “b”
RVbattery
Ca
bII++ --
-I-I
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 66
ABCD
22
Checkpoint 1cCheckpoint 1c
++--
IIRR
A circuit is wired up as shown below. The capacitor is initially uncharged and switches S1 and S2 are initially open.
After being closed a long time, switch 1 is opened and switch 2 is closed. What is the current through the right resistor immediately after switch 2 is closed?A. IR = 0 B. IR = V/3R C. IR = V/2R D. IR = V/R
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 77
V
2RCV
I
ABCD
22
Checkpoint 1cCheckpoint 1c
++--
IIRR
A circuit is wired up as shown below. The capacitor is initially uncharged and switches S1 and S2 are initially open.
After being closed a long time, switch 1 is opened and switch 2 is closed. What is the current through the right resistor immediately after switch 2 is closed?A. IR = 0 B. IR = V/3R C. IR = V/2R D. IR = V/R
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 88
ABC
26
Checkpoint 1dCheckpoint 1d
A circuit is wired up as shown below. The capacitor is initially uncharged and switches S1 and S2 are initially open.
Now suppose both switches are closed. What is the voltage across the capacitor after a very long time? A. VC = 0 B. VC = V C. VC = 2V/3
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 99
ABC
26
Checkpoint 1dCheckpoint 1d
• After both switches have been closed for a After both switches have been closed for a long timelong time
• The current through the capacitor is zeroThe current through the capacitor is zero
• The current through R = current through 2RThe current through R = current through 2R
• VVcapacitorcapacitor = V = V2R2R
• VV2R2R = 2/3 V = 2/3 V
A circuit is wired up as shown below. The capacitor is initially uncharged and switches S1 and S2 are initially open.
Now suppose both switches are closed. What is the voltage across the capacitor after a very long time? A. VC = 0 B. VC = V C. VC = 2V/3
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1010
2RC
R
S1 S2
Close both S1 and S2 andClose both S1 and S2 andwait a long time…wait a long time…
V
2RC
R
V
No current flows No current flows through the through the capacitor after a long capacitor after a long time. time. This will always This will always be the case if the be the case if the sources of EMFsources of EMFdon’t change with don’t change with time.time.
VVCC
II
I = V/(3R)I = V/(3R)
27
VV2R2R = I(2R) = (2/3)V = V = I(2R) = (2/3)V = VCC VVCC = (2/3)V = (2/3)V
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1111
DEMO – ACT 1DEMO – ACT 1
VC
S
Bulb 1Bulb 1
Bulb 2Bulb 2
What will happen after I close the switch?What will happen after I close the switch?
A)A) Both bulbs come on and stay on.Both bulbs come on and stay on.B)B) Both bulbs come on but then bulb 2 fades out.Both bulbs come on but then bulb 2 fades out.C)C) Both bulbs come on but then bulb 1 fades out.Both bulbs come on but then bulb 1 fades out.D)D) Both bulbs come on and then both fade out.Both bulbs come on and then both fade out.
R
R
30
No initial charge No initial charge on capacitoron capacitor V(bulb 1) = V(bulb 2) = VV(bulb 1) = V(bulb 2) = V Both bulbs lightBoth bulbs light
No final current No final current through capacitorthrough capacitor
V(bulb 2) = 0V(bulb 2) = 0
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1212
DEMO – ACT 2DEMO – ACT 2
VC
S
Bulb 1Bulb 1
Bulb 2Bulb 2
Suppose the switch has been closed a long time.Suppose the switch has been closed a long time.Now what will happen after open the switch?Now what will happen after open the switch?
A)A) Both bulbs come on and stay on.Both bulbs come on and stay on.B)B) Both bulbs come on but then bulb 2 fades out.Both bulbs come on but then bulb 2 fades out.C)C) Both bulbs come on but then bulb 1 fades out.Both bulbs come on but then bulb 1 fades out.D)D) Both bulbs come on and then both fade out.Both bulbs come on and then both fade out.
R
R
32
Capacitor has charge (=CV)Capacitor has charge (=CV) Capacitor discharges through both resistorsCapacitor discharges through both resistors
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1313
CalculationCalculationIn this circuit, assume V, C, and Ri are known.C initially uncharged and then switch S is closed.
What is the voltage across the capacitor What is the voltage across the capacitor after a long time ?after a long time ?
– Circuit behavior described by Kirchhoff’s Rules: • KVR: Vdrops = 0 • KCR: Iin = iout
– S closed and C charges to some voltage with some time constant
– Determine currents and voltages in circuit a long time after S closed
V
R1 R2
C
R3
S
35
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1414
CalculationCalculation
V
R1 R2
C
R3
S
Immediately after S is closed: what is I2, the current through C
what is VC, the voltage across C?
(A) (A) Only I2 = 0 (B) (B) Only VC = 0 (C) (C) Both I2 and VC = 0 (D) (D) Neither I2 nor VC = 0
• Why?– We are told that C is initially uncharged (V = Q/C)– I2 cannot be zero because charge must flow in order to charge C
In this circuit, assume V, C, and Ri are known.C initially uncharged and then switch S is closed.
What is the voltage across the capacitor What is the voltage across the capacitor after a long time ?after a long time ?
37
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1515
CalculationCalculation
V
R1 R2
C
R3
S
• Why?– Draw circuit just after S closed
(knowing VC = 0)
• Immediately after S is closed, what is I1, the current through R1 ?
V
R1 R2
S
R3
VC = 0
I1
– R1 is in series with the parallel combination of R2 and R3
In this circuit, assume V, C, and Ri are known.C initially uncharged and then switch S is closed.
What is the voltage across the capacitor What is the voltage across the capacitor after a long time ?after a long time ?
39
(A) (B) (C) (D) (E)(A) (B) (C) (D) (E)
1 3
V
R R1
V
R1 2 3
V
R R R 1 2 3
1 2 2 3 1 3
R R RVR R R R R R
32
321 RR
RRR
V
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1616
CalculationCalculation
V
R1 R2
C
R3
S
• Why?– After a long time in a static
circuit, the current through any capacitor approaches 0 !
– This means we redraw circuit with open circuit in middle leg
After S has been closed “for a long time”, what is IC, the current through C ?
(A) (B) (C)(A) (B) (C)
1
V
R 0
V
R1
R3IC = 0 VC
I
In this circuit, assume V, C, and Ri are known.C initially uncharged and then switch S is closed.
What is the voltage across the capacitor What is the voltage across the capacitor after a long time ?after a long time ?
2
V
R
41
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1717
CalculationCalculation
V
R1 R2
C
R3
S
• Why??
After S has been closed “for a long time”, what is VC, the voltage across C ?
(A) (B) (C) (D) (E)(A) (B) (C) (D) (E)
V3
1 3
RVR R 0
2
2 31
2 3
RV
R RR
R R
2
1 2
RVR R
– VC = V3 = IR3 = (V/(R1+R3))R3
In this circuit, assume V, C, and Ri are known.C initially uncharged and then switch S is closed.
What is the voltage across the capacitor What is the voltage across the capacitor after a long time ?after a long time ?
V
R1
R3VC
I I
43
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1818
ChallengeChallengeIn this circuit, assume V, C, and Ri are known.C initially uncharged and then switch S is closed.
V
R1 R2
C
R3
S
• Strategy– Write down KVR and KCR for the circuit when S is closed
• 2 loop equations and 1 node equation – Use I2 = dQ2/dt to obtain one equation that looks like simple
charging RC circuit ( (Q/”C”) + “R”(dQ/dt) – “V” = 0 )– Make correspondence: “R” = ?, and “C” = ?, then = “R” ”C”
What is c, the charging time constant?
We get: CRR
RRRc
31
312
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 1919
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 1 2 3 4 5 6 7 8 9 10
0
Q t
Q
0
t
RCQ t Q e
t
RC
““Fraction of initial Fraction of initial charge that remains”charge that remains”
““How many time constants worth How many time constants worth of time that have elapsed”of time that have elapsed”
45
How do exponentials work?How do exponentials work?
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 2020
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 1 2 3 4 5 6 7 8 9 10
0
Q t
Q
t
RC = 1
RC = 2
Time constant:Time constant: = = RCRC
The bigger The bigger is, is,the longer it takes to getthe longer it takes to getthe same change…the same change…
0
t
RCQ t Q e
47
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 2121
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 1 2 3 4 5 6 7 8 9 10
RC = 1
RC = 2
Which circuit has the largest time constant?
A) Circuit 1
B) Circuit 2
C) Same
49
= R= RequivequivCC
Checkpoint 2aCheckpoint 2a
The two circuits shown below contain identical capacitors that hold the same charge at t = 0. Circuit 2 has twice as much resistance as circuit 1.
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 222250
Checkpoint 2bCheckpoint 2b
The two circuits shown below contain identical capacitors that hold the same charge at t = 0. Circuit 2 has twice as much resistance as circuit 1.
Which of the following statements best describes the charge remaining on each of the the two capacitors for any time after t = 0?A. Q1 < Q2 B. Q1 > Q2 C. Q1 = Q2 D. Q1 < Q2 at first, then Q1 > Q2 after long time E. Q1 > Q2 at first, then Q1 < Q2 after long time
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 232350
Checkpoint 2bCheckpoint 2b
The two circuits shown below contain identical capacitors that hold the same charge at t = 0. Circuit 2 has twice as much resistance as circuit 1.
Which of the following statements best describes the charge remaining on each of the the two capacitors for any time after t = 0?A. Q1 < Q2 B. Q1 > Q2 C. Q1 = Q2 D. Q1 < Q2 at first, then Q1 > Q2 after long time E. Q1 > Q2 at first, then Q1 < Q2 after long time
Which of the following statements best describes the charge remaining on each of the the two capacitors for any time after t = 0?A. Q1 < Q2 B. Q1 > Q2 C. Q1 = Q2 D. Q1 < Q2 at first, then Q1 > Q2 after long time E. Q1 > Q2 at first, then Q1 < Q2 after long time
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 2424
Checkpoint 2bCheckpoint 2b
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 1 2 3 4 5 6 7 8 9 10
RC = 1
RC = 2
Q = QQ = Q00ee-t/RC-t/RC
Look at plot !!!Look at plot !!!
The two circuits shown below contain identical capacitors that hold the same charge at t = 0. Circuit 2 has twice as much resistance as circuit 1.
Checkpoint 2bCheckpoint 2b
Physics 212 Lecture 8, Slide Physics 212 Lecture 8, Slide 2525
Charge capacitor – store a logical “1”Charge capacitor – store a logical “1”
Discharge capacitor – store a logical “0”Discharge capacitor – store a logical “0”
Capacitor Capacitor dischargesdischarges through resistance through resistance between plates. between plates.
Only holds Q for < 1 msec.Only holds Q for < 1 msec.
““Dynamic” random access memoryDynamic” random access memory
Charge Q must be “refreshed” constantly, Charge Q must be “refreshed” constantly, So memory is called dynamic.So memory is called dynamic.
Physics 212 Lecture 11, Slide Physics 212 Lecture 11, Slide 2626
1. Capacitor is an open circuit for dc (direct current). 1. Capacitor is an open circuit for dc (direct current).
R
+Q+Q
V CIC
-Q-Q
VVCC = Q/C and I = Q/C and ICC = dQ/dt. If I = dQ/dt. If ICC isis flowing then Q is changing, so V flowing then Q is changing, so VCC is changing. is changing.
But in a dc circuit, nothing changes with time, so we must have IBut in a dc circuit, nothing changes with time, so we must have ICC = 0. = 0.
For t For t
V C
R
IC = 0
VVCC = V = V
Situation once things stop changing.Situation once things stop changing.