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Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11...

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Electricity & Magnetism Lecture 11 Today’s Concept: RC Circuits Electricity & Magne7sm Lecture 11, Slide 1
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Page 1: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

Electricity & MagnetismLecture 11

Today’s  Concept:

  RC  Circuits

Electricity  &  Magne7sm    Lecture  11,  Slide  1

Page 2: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

RC Circuit (Charging)

Kirchhoff’s  Voltage  Rule

Short  Term    (q  =  q0 =  0)

Long  Term    (Ic = 0)

RVbattery

Ca

b

Intermediate

a

RVbattery

C

b

Capacitor  uncharged,  Switch  is  moved  to  posi?on  “a”

Electricity  &  Magne7sm    Lecture  11,  Slide  2

Page 3: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

CheckPoints 2 & 4

Close  S1,  V1  =  voltage  across  C  immediately  a@er

V2  =  voltage  across  C  a  long  7me  a@er

A)      V1 = V V2 = VB)      V1  = 0 V2 = VC)      V1 = 0 V2 = 0

D)      V1 = V V2 = 0

Electricity  &  Magne7sm    Lecture  11,  Slide  3

Page 4: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

Kirchhoff’s  Voltage  Rule

Short  Term    (q = q0)

Long  Term    (Ic = 0)

RC Circuit (Discharging)

RVbattery

Ca

b

IntermediateV

Capacitor  has  q0 = CV,  Switch  is  moved  to  posi?on  “b”

RVbattery

Ca

bI+ −

−I

Electricity  &  Magne7sm    Lecture  11,  Slide  4

Page 5: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

+

CheckPoint 6

ABCD

Electricity  &  Magne7sm    Lecture  11,  Slide  5

Page 6: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

ABC

CheckPoint 8

Electricity  &  Magne7sm    Lecture  11,  Slide  6

Page 7: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

What  will  happen  aFer  I  close  the  switch?

A)    Both  bulbs  come  on  and  stay  on.B)    Both  bulbs  come  on  but  then  bulb  2  fades  out.C)    Both  bulbs  come  on  but  then  bulb  1  fades  out.D)    Both  bulbs  come  on  and  then  both  fade  out.

VC

S

Bulb  1

Bulb  2

R

R

DEMO – Clicker Question 1

Electricity  &  Magne7sm    Lecture  11,  Slide  8

Page 8: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

Suppose  the  switch  has  been  closed  a  long  ?me.Now  what  will  happen  aFer  open  the  switch?

A)  Both  bulbs  come  on  and  stay  on.B)  Both  bulbs  come  on  but  then  bulb  2  fades  out.C)  Both  bulbs  come  on  but  then  bulb  1  fades  out.D)  Both  bulbs  come  on  and  then  both  fade  out.

VC

S

Bulb  1

Bulb  2

R

R

DEMO – Clicker Question 2

Electricity  &  Magne7sm    Lecture  11,  Slide  9

Page 9: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

In  this  circuit,  assume  V, C,  and  Ri  are  known.

C  ini7ally  uncharged  and  then  switch  S  is  closed.  

What  is  the  voltage  across  the  capacitor  a@er  a  long  7me  ?

 Conceptual  Analysis:    Circuit  behavior  described  by  Kirchhoff’s  Rules:    

KVR: Σ Vdrops = 0 KCR: Σ Iin = Σ Iout

S  closed  and  C  charges  to  some  voltage  with  some  7me  constant

Strategic  AnalysisDetermine  currents  and  voltages  in  circuit  a  long  7me  a@er  S  closed

Calculation

Electricity  &  Magne7sm    Lecture  11,  Slide  10

Page 10: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

V

R1 R2

CR3

S

 Immediately  a@er  S  is  closed:        what  is  I2,  the  current  through  C      what  is  VC,  the  voltage  across  C?

A)    Only  I2 = 0 B)  Only  VC = 0 C)  Both  I2 and  VC = 0 D)  Neither I2 nor  VC = 0

 Why?We  are  told  that  C  is  ini7ally  uncharged  (V = Q/C)I2  cannot  be  zero  because  charge  must  flow  in  order  to  charge  C

CalculationIn  this  circuit,  assume  V,  C,  and  Ri are  known.C  ini7ally  uncharged  and  then  switch  S  is  closed.  

What  is  the  voltage  across  the  capacitor  a@er  a  long  7me  ?

Electricity  &  Magne7sm    Lecture  11,  Slide  11

Page 11: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

V

R1 R2

C

R3

S

 Immediately  a@er  S  is  closed,  what  is  I1,  the  current  through  R1  ?

I1

CalculationIn  this  circuit,  assume  V,  C,  and  Ri are  known.C  ini7ally  uncharged  and  then  switch  S  is  closed.  

What  is  the  voltage  across  the  capacitor  a@er  a  long  7me  ?

Electricity  &  Magne7sm    Lecture  11,  Slide  12

A                                            B                                          C                                                D                                                              E

Page 12: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

Calculation

V

R1 R2

CR3

S

A@er  S  has  been  closed  “for  a  long  7me”,  what  is  IC,  the  current  through  C  ?

A                                    B                                        C

In  this  circuit,  assume  V,  C,  and  Ri are  known.C  ini7ally  uncharged  and  then  switch  S  is  closed.  

What  is  the  voltage  across  the  capacitor  a@er  a  long  7me  ?

Electricity  &  Magne7sm    Lecture  11,  Slide  13

Page 13: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

V

R1 R2

CR3

S In  this  circuit,  assume  V,  C,  and  Ri are  known.C  ini7ally  uncharged  and  then  switch  S  is  closed.  

What  is  the  voltage  across  the  capacitor  a@er  a  long  7me  ?

Calculation

Electricity  &  Magne7sm    Lecture  11,  Slide  14

 A@er  S  has  been  closed  “for  a  long  7me”,  what  is  VC,  the  voltage  across  C  ?

     A                                      B                              C                                            D                                      E

Page 14: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

Q(t) = Q0e�t/RC

0

0.2500

0.5000

0.7500

1.0000

0 2.5000 5.0000 7.5000 10.0000

“Frac?on  of  ini?al  charge  that  remains”

“How  many  ?me  constants  worth  of  ?me  that  have  elapsed”

How do Exponentials Work?

Electricity  &  Magne7sm    Lecture  11,  Slide  16

Page 15: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

Q(t) = Q0e�t/RC

0

0.2500

0.5000

0.7500

1.0000

0 2.5000 5.0000 7.5000 10.0000

RC = 1

RC = 2

Time  constant:τ =  RC

The  bigger τ is,the  longer  it  takes  to  getthe  same  change…

Electricity  &  Magne7sm    Lecture  11,  Slide  17

Page 16: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

Which  circuit  has  the  largest  7me  constant?

A)  Circuit  1

B)  Circuit  2

C)  Same

CheckPoint 10

Electricity  &  Magne7sm    Lecture  11,  Slide  18

Page 17: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

CheckPoint 12

Electricity  &  Magne7sm    Lecture  11,  Slide  20

ABCDE

Page 18: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

0.47 µF Capacitors

Please  do  not  discharge  them  abruptly  through  a  short.

Put  a  10  Ω  resistor  across  the  terminals  if  you  wish  to  discharge  them.

Page 19: Electricity & Magnetism Lecture 11 - SFU.ca Lecture 11 - RC Circuits.pdfLecture 11 Today’s(Concept: (RC#Circuits Electricity(&(Magne7sm((Lecture(11,(Slide(1. RC Circuit (Charging)

Session 3

We  don’t  have  7me  to  do  session  3  this  semester.

Please  record  BOTH  Charge  and  Discharge  curves  for  your  circuit.  (Ac7vity  24-­‐8)

You  can  save  7me  by  figng  your  data  in  Logger  Pro.

Use  the  “Analyze”  func7on  under  the  menus.

a

RVbattery

C

b

(e) What happens to the potential difference across the

resistor at the same time? Explain.

(f) If the potential across the resistor starts to change what

must happen to the current in the circuit? Explain.

(g) Why does the draining of charge from the capacitor

eventually stop? Why does the current in the circuit go to

zero?

50 min

Capacitor Charging

If the resistor, R, in Figure 24-12 is moved up next to

the battery as shown in Figure 24-13, an uncharged

capacitor, C, can be charged by the battery in the

presence of the resistor. The qualitative and

V

Cq i

i

Two-way!

switch

R

Figure 24-13

quantitative considerations of this situation are very

analogous to that of capacitor decay. For example, the

capacitor charges up more rapidly at first when there

Page 24-26 Workshop Physics II Activity Guide SFU

© 1990-93 Dept. of Physics and Astronomy, Dickinson College Supported by FIPSE (U.S. Dept. of Ed.)

and NSF. Modified at SFU by S. Johnson, 2008.

Text

Use this Instead of this


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