Midterm Tufree Physics II

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    GENERAL PHYSICS II

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    1 Electro StaticsCoulomb

    s law

    rR

    QkQF

    2

    21

    1. 4 4 4

    A.(3),(1),(2),(4) B.(4),(2),(1),(3)

    C.(2),(3),(4),(1) D.(1),(4),(3),(2)

    E.(3),(4),(1),(2)

    3. 4 2

    A.(a),(b),(v),(d) B.(a),(b),(c)

    C.(a),(b) D.(a)

    E.(b),(c),(d)

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    GENERAL PHYSICS II

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    2 Charge is Quantized

    Q (C)N e

    = -1.610-19C

    3 The Electric Field

    rR

    kQE

    2

    Electric Dipole

    Q = Ne

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    GENERAL PHYSICS II

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    4 Electric Field Continuous Charge

    Distributionr

    r

    dqkE

    2

    Volume charge density:when a charge is distributed evenly throughouta volume

    = Q/ V

    Surface charge density:when a charge is distributed evenly over asurface area

    = Q/A

    Linear charge density:when a charge is distributed along a line

    = Q/

    EX. Line Charge

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    GENERAL PHYSICS II

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    EX Charged Disk

    5 Gausss Law

    Electric fluxis the product of the magnitude of the electric field and the

    surface area,A, perpendicular to the field

    AdE

    Gauss lawrelates the net flux of an electric field through a closedsurface (a Gaussian surface) to the net charge q

    encthat is enclosed by

    that surface.

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    GENERAL PHYSICS II

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    0

    encqAdE

    EX Applying Gausss Law

    Cylindrical Symmetry

    Planar Symmetry

    Spherically Symmetric

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    GENERAL PHYSICS II

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    4.

    A. B.

    C. D.

    E.

    6. 3

    = 2.00 R= 100 cm

    7. 1.50 m

    = (3.00 4.00) 6.00 7.00

    6 Electric Potentialand Potential EnergyConsider two charged particles. The potential energy of the system is

    12

    21

    R

    QkQU

    The electric potential is

    R

    kQV

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    GENERAL PHYSICS II

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    1.

    2.

    7. Equipotential Surface A.B.C.D.E.

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    GENERAL PHYSICS II

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    Electric Field from Potential

    In general, the electric potential is a function of all three dimensions

    Given V(x,y,z) you can findEx

    ,Ey

    andEz

    as partial derivatives

    V(x,y,z) =

    1. = 3 2

    E. A D ................................................. N/C

    2. r = 3 2

    A.2.51 10NB. 5.20 10NC. 7.53 10ND. 1.00 10NE. A D ................................................. N

    3. + r = 3 2 r = 3 2 A.-1.85 10JB.1.85 10JC.-4.19 10JD.8.39 10JE. A D ................................................. J

    x y z

    V V VE E E

    x y z

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    GENERAL PHYSICS II

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    4. r = 3 2 1A.628.3 CNm /2 B.-628.3 CNm /2 C.377.0 CNm /2 D.-377.0 CNm /2 E. A D ................................................. CNm /2

    7

    Capacitance

    C (Farad;F)Q

    V

    (Combination of Capacitors)

    1. (Series Combination) Q (Q1= Q2= Q3= Q) V

    Ceq

    V

    QC

    CVQ

    ...1111

    321

    CCCCeq

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    2. (Parallel Combination) V (V1=V2= V3= V) Q

    Ceq

    1. C1=1.16 F C

    2=3.22 F V=96.9 v

    a c b d S1

    S2 C

    1,C

    2 e f

    1. C1= C

    5= 8.4 C

    2= C

    3=C

    4= 4.2 V

    ab= 220

    ...321 CCCCeq

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    A. a b 2.5

    B. C1 5.5 x 10-4

    C. V5= 66V voltage C5

    D. A,B,C

    E. A,B,C

    Capacitors with Dielectrics

    A dielectricis a nonconducting material that, when placed between the plates ofa capacitor, increases the capacitance

    Dielectrics include rubber, plastic, and waxed paper

    0CC The capacitance is multiplied by the factor when the dielectric completely fillsthe region between the plates.

    W (J)V (Volt)

    QVW2

    1

    2

    2

    1CVW

    C

    QW

    2

    2

    1

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    6. a,b =

    Electric Circuits

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    () (Q)

    (C/s) (A)Q (C)t (s)

    1 (Resistivity)

    (R)

    (Resistivity) (m)

    (m)A (m2)

    4. 6 3

    A.54

    B.55

    C.56

    D.57

    E.58

    tQI

    AR

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    2 Kirchhoffs Rules1 Junction rule

    321 III

    2 Loop rule

    A B(VAB= VA VB)

    1. 2. A B 3. A B

    I = I

    Loop Loop

    IRE

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    4.

    A. Vad

    6.58 V

    B. Vad

    4.58 V

    C. 4.00 V 3.983 V

    D. 4.00 V 4.00 VE.

    3. A

    RE

    RD

    RC

    RB

    RA

    12

    10.

    9

    8.

    7.

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    5. P 100 V Q

    A. -10V

    B.+10VC.-20V

    D.+20V

    E.+30V

    3 RC Circuits:

    Charging

    The charge on the capacitor varies with time

    q(t)= C (1 e-t/RC

    ) =Q(1 e-t/RC

    )

    The current can be found

    RCteRdt

    dqti /)(

    is the time constant = RC

    Discharging

    q(t)= Qe-t/RC

    2. RC t= 0 s 100 V,

    1.06 V 10 s t=17s A.2.2 , 44

    B.3.3 , 66

    C.4.4 , 88D.5.5 ,100

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    E.6.6 ,110

    Magnetic Fields

    1Magnetic Force

    F

    (N)

    q (C)v (m/s)B

    (T)

    v B

    2. 50 cm 2.0 N/C

    A. 5.5610-11 B. 5.5610-7

    C. 1.3910-11

    E. 2.2210-11

    BvqF

    sinBvqF

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    5. 75.0 cm 0.860 T x

    a b c d e f 6.58 A f N

    A.

    -4.24 B.-4.24 C. 4.24 D. 4.24 E. 4.24 -4.24

    B.

    (T)

    (Helical Path)

    qB

    mvR

    qB

    mT

    2

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    GENERAL PHYSICS II

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    1.

    2.

    3.

    14. 22.5 B=455 T 65.5

    A.75.6 ,1.2

    B.76.6 ,1.2

    C.77.6 ,2.2

    D.78.6 ,3.2

    E.79.9 ,3.2

    7.K d

    m e

    qB

    mvR

    sin

    qB

    mT

    2

    S

    qB

    mv

    2

    cos

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    (Magnetic Force Acting on a Current Carrying Conductor)

    F

    (N)I (A)

    (m)

    B

    (T)

    B

    BIF

    sinBIF

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    7. AB I CD AB

    C D CD

    I AB CD CD

    h

    AB

    2

    E (Volt)L (m)v (m/s) v B

    E Bv

    E = LvBsin

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    10.

    11. = 262 = 12.7 = 13 477

    A.1.33A

    B.1.44A

    C.1.55A

    D.1.66A

    E.1.78A

    3 Amperes Law

    enciSdB 0

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    Solenoids and Toroids

    r

    iNB

    2

    0

    inB0

    4 Faradays Law of Induction

    dt

    dN B

    AdBB

    Induced Electric Fields

    dt

    dSdE B

    12.

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    13. = 12, = 16

    emf = 3A.300 B.400

    C.500

    D.600

    E.660

    9.

    b

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    GENERAL PHYSICS II

    12. AB di/dt

    a)

    b) emf

    c) emf

    a=12.0 cm b=36.0 cm L=24.0 cm di/dt=9.60 A/s

    10. 4.00 cm 0.0280A 1.00 cm

    A.7.5 x 10-7T B. 6.5 x 10-7T C.5.5 x 10-7T

    D. 4.5 x 10-7T E.3.5 x 10-7T