(Capacitor) Chapter32B 1

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    Chapter 32B - RC Circuits

    A PowerPoint Presentation by

    Paul E. Tippens, Professor of Physics

    Southern Polytechnic State University

    2007

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    RC Circuits: The rise and decayof currents in capacitive circuits

    The calculus is used only for derivation of

    equations for predicting the rise and decayof charge on a capacitor in series with asingle resistance. Applications are notcalculus based.

    Check with your instructor to see if thismodule is required for your course.

    Optional: Check with Instructor

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    RC Circuit

    R

    V C

    +

    +

    --

    a

    b

    RC-Circuit: Resistance R and capacitance Cin series with a source of emf V.

    Start charging capacitor. . . loop rule gives:

    ;q

    iR V iR

    C

    E

    R

    V C

    +

    +

    --

    a

    bi

    q

    C

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    RC Circuit: Charging Capacitor

    Rearrange terms to place in differential form:

    qV iRC

    R

    V C

    +

    +

    --

    a

    bi

    qC

    dq q

    R Vdt C

    ( )RCdq CV q dt

    ( )

    dq dt

    CV q RC

    0 ( )

    q t

    o

    dq dt

    CV q RC

    Multiply by C dt :

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    RC Circuit: Charging Capacitor

    R

    V C

    +

    +

    --

    a

    bi

    qC 0 ( )

    q t

    o

    dq dt CV q RC

    0ln( )

    q t

    CV q RC

    (1/ )RC tCV q CVe

    ln( ) ln( )t

    CV q CV

    RC

    ( )ln

    CV q t

    CV RC

    /1 t RCq CV e

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    RC Circuit: Charging Capacitor

    R

    V C

    +

    +

    --

    a

    bi

    qC

    /1

    t RCq CV e

    Instantaneous charge qon a charging capacitor:

    At time t= 0: q = CV(1 - 1); q = 0

    At time t= : q = CV(1 - 0); qmax= CV

    The charge qrises from zero initially toits maximum value qmax = CV

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    Example 1. What is the charge on a 4-mFcapacitor charged by 12-V for a time t = RC?

    Time, t

    Qmax q

    Rise inCharge

    Capacitor

    t

    0.63 Q

    The time t = RCis known

    as the time constant. /1 t RCq CV e

    11q CV e

    R =1400 W

    V 4 mF

    +

    +

    --

    a

    bi

    e= 2.718; e-1= 0.63

    1 0.37q CV

    0.63q CV

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    Example 1 (Cont.) What is the time constant t?

    Time, t

    Qmax q

    Rise inCharge

    Capacitor

    t

    0.63 Q

    The time t = RCis known

    as the time constant.

    R =1400 W

    V 4 mF

    +

    +

    --

    a

    bi

    In one time constant

    (5.60 ms in thisexample), the chargerises to 63% of itsmaximum value (CV).

    t = (1400 W)(4 mF)

    t = 5.60 ms

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    RC Circuit: Decay of Current

    R

    V C

    +

    +

    --

    a

    bi

    qC

    /1 t RCq CV e

    As charge qrises, thecurrent iwill decay.

    / /t RC t RC dq d CV

    i CV CVe e

    dt dt RC

    Current decay as acapacitor is charged:

    /t RCVi e

    R

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    Current Decay

    Time, t

    I i

    CurrentDecay

    Capacitor

    t

    0.37 I

    R

    V C

    +

    +

    --

    a

    bi

    qC

    The current is a maximum

    of I = V/R when t = 0.The current is zero whent = (because the backemf from C is equal to V).

    /t RCVi e

    R

    Consider i when

    t = 0 and t = .

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    Example 2. What is the current iafter one timeconstant (t RC)? Given Rand Cas before.

    The time t = RCis known

    as the time constant.

    e= 2.718; e-1= 0.37

    max0.37 0.37V

    i iR

    R =1400 W

    V 4 mF

    +

    +

    --

    a

    bi

    Time, t

    I i

    CurrentDecay

    Capacitor

    t

    0.37 I

    / 1t RCV Vi e e

    R C

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    Charge and Current During theCharging of a Capacitor.

    Time, t

    Qmaxq

    Rise in

    Charge

    Capacitor

    t

    0.63 I

    Time, t

    Ii

    Current

    Decay

    Capacitor

    t

    0.37 I

    In a time t of one time constant, the charge qrises to 63% of its maximum, while the current idecays to 37% of its maximum value.

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    RC Circuit: Discharge

    R

    V C

    +

    +

    --

    a

    b

    After C is fully charged, we turn switch tob, allowing it to discharge.

    Discharging capacitor. . . loop rule gives:

    ;q

    iR iR

    C

    E

    R

    V C

    +

    +

    --

    a

    bi

    q

    C

    Negative becauseof decreasing I.

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    Discharging From q0 to q:

    ;dq

    q RCi q RC

    dt

    Instantaneous charge qon discharging capacitor:

    R

    V C

    +

    +

    --

    a

    bi

    qC

    ;dq dt

    q RC

    0 0

    ;q t

    q

    dq dt

    q RC

    00

    ln

    tq

    q

    tq

    RC

    0ln lnt

    q qRC

    0

    lnq t

    q RC

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    Discharging Capacitor

    R

    V C

    +

    +

    --

    a

    bi

    q

    C0

    ln

    q t

    q RC

    /

    0

    t RCq q e

    Note qo = CV and the instantaneous current is: dq/dt.

    / /t RC t RC dq d CV

    i CVe edt dt RC

    /t RCVi e

    C

    Current ifor a

    discharging capacitor.

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    Prob. 45. How many time constants are neededfor a capacitor to reach 99% of final charge?

    R

    V C

    +

    +

    --

    a

    bi

    qC /max 1 t RCq q e

    /

    max

    0.99 1t RCq

    eq

    Let x = t/RC, then: e-x = 1-0.99 or e-x = 0.01

    1 0.01; 100xx

    ee

    ln (100)e xFrom definitionof logarithm:

    x= 4.61t

    x

    RC

    4.61 timeconstants

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    Prob. 46. Find time constant, qmax, and time toreach a charge of16 mC ifV= 12 V and C= 4 mF.

    /max 1 t RCq q e R

    V

    1.8 mF

    +

    +

    --

    a

    bi

    1.4 MW

    C12 V

    t = RC = (1.4 MW)(1.8 mF)

    t = 2.52 s

    qmax = CV = (1.8 mF)(12 V); qmax = 21.6 mC

    /

    max

    16 C1

    21.6 C

    t RCqe

    q

    m

    m

    /1 0.741t RC

    e

    Continued . . .

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    Prob. 46. Find time constant, qmax, and time toreach a charge of16 mC ifV= 12 V and C= 4 mF.

    R

    V

    1.8 mF

    +

    +

    --

    a

    bi

    1.4 MW

    C12 V

    /1 0.741t RCe

    Let x = t/RC, then:

    1 0.741 0.259xe 1

    0.259; 3.86x

    xe

    e ln (3.86)e x

    From definitionof logarithm:

    x= 1.35 1.35; (1.35)(2.52s)t tRC

    t= 3.40 sTime to reach 16 mC:

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    CONCLUSION: Chapter 32B

    RC Circuits