ap lecture ch 16

Upload: theresatco

Post on 06-Apr-2018

220 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/3/2019 AP Lecture Ch 16

    1/59

    January 19, 2012

    Notes on Electric Charge (R2)

    Question of the Day (L1):

    Explain why the balloons repel each other?

  • 8/3/2019 AP Lecture Ch 16

    2/59

    Chapter 16

    Electric Charge andElectric Field

  • 8/3/2019 AP Lecture Ch 16

    3/59

    16.1 Static Electricity;

    Electric Charge and Its

    Conservation

    Charge comes in two

    types, positive andnegative; like charges

    repel and opposite

    charges attract

  • 8/3/2019 AP Lecture Ch 16

    4/59

    16.1 Static Electricity; Electric Charge

    and Its Conservation

    Electric charge is conserved the

    arithmetic sum of the total charge cannotchange in any interaction.

  • 8/3/2019 AP Lecture Ch 16

    5/59

    16.2 Electric Charge in the Atom

    Atom:

    Nucleus (small,

    massive, positive

    charge)Electron cloud (large,

    very low density,

    negative charge)

  • 8/3/2019 AP Lecture Ch 16

    6/59

    16.2 Electric Charge in the Atom

    Atom is electrically neutral.

    Rubbing charges objects by moving electrons

    from one to the other.

  • 8/3/2019 AP Lecture Ch 16

    7/59

    Question

    Why do the balloons eventually lose charge

    and no longer repel?

  • 8/3/2019 AP Lecture Ch 16

    8/59

    16.2 Electric Charge in the Atom

    Polar molecule: neutral overall, but charge not

    evenly distributed

  • 8/3/2019 AP Lecture Ch 16

    9/59

    16.3 Insulators and Conductors

    Conductor:

    Charge flows freely

    Metals

    Insulator:

    Almost no charge flows

    Most other materials

    Some materials are semiconductors.

  • 8/3/2019 AP Lecture Ch 16

    10/59

    16.4 Induced Charge

    Metal objects can be charged by conduction:

  • 8/3/2019 AP Lecture Ch 16

    11/59

    16.4 Induced Charge

    They can also be charged by induction:

  • 8/3/2019 AP Lecture Ch 16

    12/59

    16.4 Induced Charge

    Nonconductors wont become charged byconduction or induction, but will experience

    charge separation:

  • 8/3/2019 AP Lecture Ch 16

    13/59

    16.4 Electroscope

    The electroscopecan be used for

    detecting charge:

  • 8/3/2019 AP Lecture Ch 16

    14/59

    16.4 Electroscope

    The electroscope can be charged either by

    conduction or by induction.

  • 8/3/2019 AP Lecture Ch 16

    15/59

    16.4 Electroscope

    The charged electroscope can then be used todetermine the sign of an unknown charge.

  • 8/3/2019 AP Lecture Ch 16

    16/59

    January 20, 2012

    ConcepTest Review

    Coulombs Law (R3)

    Practice Problems

    Question of the Day (L2):

    Whats behind the phenomena of these

    demonstrations? Explain.

  • 8/3/2019 AP Lecture Ch 16

    17/59

    1) have opposite charges

    2) have the same charge

    3) all have the same charge

    4) one ball must be neutral (no charge)

    From theFrom the

    picture, whatpicture, whatcan youcan you

    conclude aboutconclude about

    the charges?the charges?

  • 8/3/2019 AP Lecture Ch 16

    18/59

    1) have opposite charges

    2) have the same charge

    3) all have the same charge

    4) one ball must be neutral (no charge)

    From theFrom the

    picture, whatpicture, whatcan youcan you

    conclude aboutconclude about

    the charges?the charges?

    The TAN and PURPLE balls must

    have the same charge, since they

    repel each other. TheYELLOW

    ball also repels the TAN, so it must

    also have the same charge as the

    TAN (and the PURPLE).

  • 8/3/2019 AP Lecture Ch 16

    19/59

    Ametal ball hangs from the

    ceiling by an insulating thread.

    The ball is attracted to a positive-

    charged rod held near the ball.

    The charge of the ball must be:

    1) positive

    2) negative

    3) neutral

    4) positive or neutral

    5) negative or neutral

  • 8/3/2019 AP Lecture Ch 16

    20/59

    Clearly, the ball will be attracted if its

    charge is negativenegative. However, even if

    the ball is neutralneutral, the charges in theball can be separated by inductioninduction

    (polarization), leading to a net

    attraction.

    1) positive

    2) negative

    3) neutral

    4) positive or neutral

    5) negative or neutral

    Ametal ball hangs from the

    ceiling by an insulating thread.

    The ball is attracted to a positive-

    charged rod held near the ball.

    The charge of the ball must be:

    rememberthe ball is aconductor!

    FollowFollow--up:up: What happens if theWhat happens if the metal ballmetal ball is replaced by ais replaced by a plastic ballplastic ball??

  • 8/3/2019 AP Lecture Ch 16

    21/59

    Two neutral conductors are connected

    by a wire and a charged rod is brought

    near, but does not touch. The wire is

    taken away, and then the charged rod is

    removed. What are the charges on the

    conductors?

    1) 0 0

    2) +

    3) +

    4) + +

    5)

    0 0

    ? ?

  • 8/3/2019 AP Lecture Ch 16

    22/59

    While the conductors are connected,positivepositive

    charge will flow from the blue to the greencharge will flow from the blue to the green

    ball due to polarizationball due to polarization. Once disconnected,

    the charges will remain on the separatecharges will remain on the separate

    conductorsconductors even when the rod is removed.

    Two neutral conductors are connected

    by a wire and a charged rod is broughtnear, but does not touch. The wire is

    taken away, and then the charged rod is

    removed. What are the charges on the

    conductors?

    1) 0 0

    2) +

    3) +

    4) + +

    5)

    0 0

    ? ?

    FollowFollow--up:up: What will happen when theWhat will happen when the

    conductors are reconnected with a wire?conductors are reconnected with a wire?

  • 8/3/2019 AP Lecture Ch 16

    23/59

    16.5 Coulombs Law

    Experiment shows that the electric forcebetween two charges is proportional to the

    product of the charges and inversely

    proportional to the distance between them.

  • 8/3/2019 AP Lecture Ch 16

    24/59

    16.5 Coulombs Law

    Coulombs law:

    (16-1)

    This equation gives the magnitude of

    the force.

  • 8/3/2019 AP Lecture Ch 16

    25/59

    16.5 Coulombs Law

    The force is along the line connecting the

    charges, and is attractive if the charges areopposite, and repulsive if they are the same.

  • 8/3/2019 AP Lecture Ch 16

    26/59

    16.5 Coulombs Law

    Unit of charge: coulomb, C

    The proportionality constant in Coulombs

    law is then:

    Charges produced by rubbing are

    typically around a microcoulomb:

  • 8/3/2019 AP Lecture Ch 16

    27/59

    16.5 Coulombs Law

    Charge on the electron:

    Electric charge is quantized in units

    of the electron charge.

  • 8/3/2019 AP Lecture Ch 16

    28/59

    16.5 Coulombs Law Practice

    Calculate the magnitude of the forcebetween two point charges 9.3 cm

    apart.

    C-60.3 Q

  • 8/3/2019 AP Lecture Ch 16

    29/59

    16.5 Coulombs Law Practice

    Calculate the magnitude of the forcebetween two point charges 9.3 cm

    apart.

    C-60.3 Q

    26

    9 2 21 2

    222

    3.60 10 C

    8.988 10 N m C 13.47 N 13 N9.3 10 m

    Q Q

    F k r

    v

    ! ! v ! }v

  • 8/3/2019 AP Lecture Ch 16

    30/59

    Opening Question: Practice

    How many electrons make up a charge of

    C?0.30 Q

  • 8/3/2019 AP Lecture Ch 16

    31/59

    16.5 Coulombs Law Practice

    How many electrons make up a charge of

    C?0.30 Q

    6 14

    19

    1 electron30.0 10 C 1.87 10 electrons

    1.602 10 C

    v ! v v

  • 8/3/2019 AP Lecture Ch 16

    32/59

    16.5 Coulombs Law

    The proportionality constant kcan also bewritten in terms of , the permittivity of free

    space:

    (16-2)

  • 8/3/2019 AP Lecture Ch 16

    33/59

    16.5 Coulombs Law

    Coulombs law strictly applies only to point charges.

    Superposition: for multiple point charges, the forceson each charge from every other charge can be

    calculated and then added as vectors.

  • 8/3/2019 AP Lecture Ch 16

    34/59

    16.6 Solving Problems Involving

    Coulombs Law and Vectors

    The net force on a charge is the vector

    sum of all the forces acting on it.

  • 8/3/2019 AP Lecture Ch 16

    35/59

    16.6 Solving Problems Involving

    Coulombs Law and Vectors

    Vector addition review:

  • 8/3/2019 AP Lecture Ch 16

    36/59

    16.5 Coulombs Law Practice

    Three charged particles are placed at thecorners of an equilateral triangle of side 1.20

    m (Fig. 1653). The charges are

    and Calculate the magnitude and

    direction of the net force on each due to theother two.

    C,0.8C,0.4 QQ

    C.0.6 Q

  • 8/3/2019 AP Lecture Ch 16

    37/59

    16.5 Coulombs Law Practice

    1Q

    2Q

    3Q

    12

    F

    &

    d

    13F

    &

    d

    d

    32F

    &

    31F

    &

    21F

    &

    23F

    &

    First draw a picture.

  • 8/3/2019 AP Lecture Ch 16

    38/59

    16.5 Coulombs Law Practice

    1Q

    2Q

    3Q

    12

    F

    &

    d

    13F

    &

    d

    d

    32F

    &

    31F

    &

    21F

    &

    23F

    &

    6 6

    9 2 21 2

    12 22

    21

    6 6

    9 2 21 3

    13 22

    31

    4.0 10 C 8.0 10 C8.988 10 N m C

    1.20 m

    0.1997 N

    4.0 10 C 6.0 10 C8.988 10 N m C

    1.20 m

    0.1498N

    Q QF k

    d

    F

    Q QF k

    d

    F

    v v! ! v

    ! !

    v v! ! v

    ! !

    Then calculate the magnitude ofeach individual force.

  • 8/3/2019 AP Lecture Ch 16

    39/59

    16.5 Coulombs Law Practice

    1Q

    2Q

    3Q

    12

    F

    &

    d

    13F

    &

    d

    d

    32F

    &

    31F

    &

    21F

    &

    23F

    &

    6 6

    9 2 21 2

    12 22

    21

    6 6

    9 2 21 3

    13 22

    31

    4.0 10 C 8.0 10 C8.988 10 N m C

    1.20 m

    0.1997 N

    4.0 10 C 6.0 10 C8.988 10 N m C

    1.20 m

    0.1498N

    Q QF k

    d

    F

    Q QF k

    d

    F

    v v! ! v

    ! !

    v v! ! v

    ! !

    First calculate the magnitude of eachindividual force.

  • 8/3/2019 AP Lecture Ch 16

    40/59

    16.5 Coulombs Law Practice

    1Q

    2Q

    3Q

    12

    F

    &

    d

    13F

    &

    d

    d

    32F

    &

    31F

    &

    21F

    &

    23F

    &

    6 6

    9 2 21 2

    12 22

    21

    6 6

    9 2 21 3

    13 22

    31

    4.0 10 C 8.0 10 C8.988 10 N m C

    1.20 m

    0.1997 N

    4.0 10 C 6.0 10 C8.988 10 N m C

    1.20 m

    0.1498N

    Q QF k

    d

    F

    Q QF k

    d

    F

    v v! ! v

    ! !

    v v! ! v

    ! !

    6 6

    9 2 22 3

    23 3222

    8.0 10 C 6.0 10 C8.988 10 N m C 0.2996 N

    1.20 m

    Q Q F k F

    d

    v v! ! v ! !

    First calculate the magnitude of eachindividual force.

  • 8/3/2019 AP Lecture Ch 16

    41/59

    16.5 Coulombs Law Practice

    Now calculate the net force on each charge

    o o 2

    1 12 13

    o o 1

    1 12 13

    1

    12 2 1 1 o

    1 1 1 1 2

    1

    0.1997 N cos 60 0.1498N cos 60 2.495 10 N

    0.1997 N sin 60 0.1498N sin 60 3.027 10 N

    3.027 10 N

    0.30 N tan tan 2652.495 10 N

    x x x

    y y y

    y

    x y

    x

    F F F

    F F F

    F

    F F F FU

    ! ! ! v

    ! ! ! v

    v

    ! ! ! ! ! v

    1Q

    2Q

    3Q

    12F

    &

    13F

    &

  • 8/3/2019 AP Lecture Ch 16

    42/59

    16.5 Coulombs Law Practice

    Now calculate direction of that net force, using

    components.

    o o 2

    13

    o o 1

    13

    1

    12 1 1 o

    1 1 2

    1

    0.1997 N cos 60 0.1498 N cos 60 2.495 10 N

    0.1997 N sin 60 0.1498N sin 60 3.027 10 N

    3.027 10 N0.30 N tan tan 2652.495 10 N

    x

    y

    y

    y

    x

    F

    F

    FFF

    U

    ! ! v

    ! ! v

    v ! ! ! ! v

    1Q

    2Q

    3Q

    12F

    &

    13F

    &

  • 8/3/2019 AP Lecture Ch 16

    43/59

    16.7 The Electric Field

    The electric field is theforce on a small charge,

    divided by the charge:

    (16-3)

  • 8/3/2019 AP Lecture Ch 16

    44/59

    16.7 The Electric Field

    For a point charge:

    (16-4a)

    (16-4b)

  • 8/3/2019 AP Lecture Ch 16

    45/59

    16.7 The Electric Field

    Force on a point charge in an electric field:

    (16-5)

    Superposition principle for electric fields:

  • 8/3/2019 AP Lecture Ch 16

    46/59

    16.7 The Electric Field

    Problem solving in electrostatics: electricforces and electric fields

    1. Draw a diagram; show all charges, with

    signs, and electric fields and forces with

    directions

    2. Calculate forces using Coulombs law

    3. Add forces vectorially to get result

  • 8/3/2019 AP Lecture Ch 16

    47/59

    16.8 Field Lines

    The electric field can be represented by field

    lines. These lines start on a positive charge

    and end on a negative charge.

  • 8/3/2019 AP Lecture Ch 16

    48/59

    16.8 Field Lines

    The number of field lines starting (ending)

    on a positive (negative) charge is

    proportional to the magnitude of the charge.

    The electric field is stronger where the field

    lines are closer together.

  • 8/3/2019 AP Lecture Ch 16

    49/59

    16.8 Field Lines

    Electric dipole: two equal charges, opposite insign:

  • 8/3/2019 AP Lecture Ch 16

    50/59

    16.8 Field Lines

    The electric field between

    two closely spaced,

    oppositely charged parallel

    plates is constant.

  • 8/3/2019 AP Lecture Ch 16

    51/59

    16.8 Field Lines

    Summary of field lines:

    1. Field lines indicate the direction of the

    field; the field is tangent to the line.

    2. The magnitude of the field is proportional

    to the density of the lines.

    3. Field lines start on positive charges and

    end on negative charges; the number is

    proportional to the magnitude of thecharge.

  • 8/3/2019 AP Lecture Ch 16

    52/59

    16.9 Electric Fields and Conductors

    The static electric field inside a conductor is

    zero if it were not, the charges would move.

    The net charge on a conductor is on its

    surface.

  • 8/3/2019 AP Lecture Ch 16

    53/59

    16.9 Electric Fields and Conductors

    The electric field isperpendicular to the

    surface of a conductor

    again, if it were not,

    charges would move.

    16 12 Ph t M hi d

  • 8/3/2019 AP Lecture Ch 16

    54/59

    16.12 Photocopy Machines and

    Computer Printers Use Electrostatics

    Photocopy machine:

    drum is charged positively

    image is focused on drum

    only black areas stay charged and

    therefore attract toner particles

    image is transferred to paper and sealed by

    heat

    16 12 Ph t M hi d

  • 8/3/2019 AP Lecture Ch 16

    55/59

    16.12 Photocopy Machines and

    Computer Printers Use Electrostatics

    16 12 Ph t M hi d

  • 8/3/2019 AP Lecture Ch 16

    56/59

    16.12 Photocopy Machines and

    Computer Printers Use Electrostatics

    Laser printer is similar, except a computercontrols the laser intensity to form the image

    on the drum

    Summary of Chapter 16

  • 8/3/2019 AP Lecture Ch 16

    57/59

    Two kinds of electric charge positive andnegative

    Charge is conserved

    Charge on electron:

    Conductors: electrons free to move

    Insulators: nonconductors

    Summary of Chapter 16

    Summary of Chapter 16

  • 8/3/2019 AP Lecture Ch 16

    58/59

    Summary of Chapter 16

    Charge is quantized in units ofe

    Objects can be charged by conduction or

    induction

    Coulombs law:

    Electric field is force per unit charge:

    Summary of Chapter 16

  • 8/3/2019 AP Lecture Ch 16

    59/59

    Summary of Chapter 16

    Electric field of a point charge:

    Electric field can be represented by electric

    field lines

    Static electric field inside conductor is zero;

    surface field is perpendicular to surface

    Electric flux:

    Gausss law: