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Electrostatics

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Electrostatics * Electric Potential For a spherical or point charge, the electric potential can be calculated by the following formula V = kq/r V: potential (V) k: 9 ... – PowerPoint PPT presentation

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Title: Electrostatics


1
Electrostatics
  • October 5, 2013

2
iClicker
  • An object is placed on the axis of a converging
    thin lens of focal length 2 cm, at a distance of
    8 cm from the lens. The distance between the
    image and the lens is most nearly
  • a. 0.4 cm
  • b. 0.8 cm
  • c. 1.6 cm
  • d. 2.0 cm
  • e. 2.7 cm

3
Atomic Charges
  • The atom has positive charge in the nucleus,
    located in the protons.
  • The positive charge cannot move from the atom
    unless there is a nuclear reaction.
  • The atom has negative charge in the electron
    cloud on the outside of the atom.
  • Electrons can move from atom to atom without all
    that much difficulty.

4
Charge
  • Charge comes in two forms, which Ben Franklin
    designated as positive () and negative().
  • Charge is quantized
  • It only comes in packets
  • The smallest possible stable charge, which we
    designate as e, is the magnitude of the charge on
    1 electron or 1 proton.
  • e is referred to as the elementary charge.
  • e 1.602 10-19 Coulombs.
  • We say a proton has charge of e, and an electron
    has a charge of e.

5
Problem
  • A certain static discharge delivers -0.5 Coulombs
    of electrical charge. How many electrons are in
    this discharge?

6
Problem
  • The total charge of a system composed of 1800
    particles, all of which are protons or electrons,
    is 31x10-18 C. How many protons are in the
    system? How many electrons are in the system?

7
Coulombs Law andElectrical Force
8
Electric Force
  • Charges exert forces on each other.
  • Like charges (two positives, or two negatives)
    repel each other, resulting in a repulsive force.
  • Opposite charges (a positive and a negative)
    attract each other, resulting in an attractive
    force.

9
Coulombs Law
  • Coulombs law tells us how the magnitude of the
    force between two particles varies with their
    charge and with the distance between them.
  • k 9.0 109 N m2 / C2
  • q1, q2 are charges (C)
  • r is distance between the charges (m)
  • F is force (N)
  • Coulombs law applies directly only to
    spherically symmetric charges.

10
Problem
  • A point charge of positive 12.0 µC experiences an
    attractive force of 51 mN when it is placed 15 cm
    from another point charge. What is the other
    charge?

11
iClicker
  • Two isolated charges, q and - 2q, are 2
    centimeters apart. If F is the magnitude of the
    force acting on charge -2q, what are the
    magnitude and direction of the force acting on
    charge q ?
  • Magnitude Direction
  • (A) (1/2) F Toward charge - 2q
  • (B) 2 F Away from charge -2q
  • (C) F Toward charge - 2q
  • (D) F Away from charge - 2q
  • (E) 2F Toward charge - 2q

12
Superposition
  • Electrical force, like all forces, is a vector
    quantity.
  • If a charge is subjected to forces from more than
    one other charge, vector addition must be
    performed.
  • Vector addition to find the resultant vector is
    sometimes called superposition.

13
Problem
14
Electric Fields
15
The Electric Field
  • The presence of or charge modifies empty
    space. This enables the electrical force to act
    on charged particles without actually touching
    them.
  • We say that an electric field is created in the
    space around a charged particle or a
    configuration of charges.
  • If a charged particle is placed in an electric
    field created by other charges, it will
    experience a force as a result of the field.
  • We can easily calculate the electric force from
    the electric field.

16
Electric Fields
  • Forces exist only when two or more particles are
    present.
  • Fields exist even if no force is present.

17
Field Lines Around Charges
  • The arrows in a field are not vectors, they are
    lines of force.
  • The lines of force indicate the direction of the
    force on a positive charge placed in the field.
  • Negative charges experience a force in the
    opposite direction.

18
Field Line Rules
19
Single Charges
20
Double Charges
21
Plate Charges
22
Field Vectors from Field Lines
  • The electric field at a given point is not the
    field line itself, but can be determined from the
    field line.
  • The electric field vectors, and thus force
    vector, is always tangent to the line of force at
    that point.

23
Force due to Electric Field
  • The force on a charged particle placed in an
    electric field is easily calculated.
  • F Eq
  • F Force (N)
  • E Electric Field (N/C)
  • q Charge (C)

24
Problem
  • The electric field in a given region is 4000 N/C
    pointed toward the north. What is the force
    exerted on a 400 µg Styrofoam bead bearing 600
    excess electrons when placed in the field? Ignore
    gravitational effects.

25
iClicker
  • An electron e and a proton p are simultaneously
    released from rest in a uniform electric field E.
    Assume that the particles are sufficiently far
    apart so that the only force acting on each
    particle after it is released is that due to the
    electric field. At a later time when the
    particles are still in the field, the electron
    and the proton will have the same
  • a. direction of motion
  • b. speed
  • c. displacement
  • d. magnitude of acceleration
  • e. magnitude of force acting on them

26
Problem
  • A 400 mg Styrofoam bead has 600 excess electrons
    on its surface. What is the magnitude and
    direction of the electric field that will suspend
    the bead in midair?

27
Problem
  • A proton traveling at 440 m/s in the x direction
    enters an electric field of magnitude 5400 N/C
    directed in the y direction. Find the
    acceleration.

28
Electric Fields
  • The Electric Field surrounding a point charge or
    a spherical charge can be calculated by
  • E kq / r2
  • E Electric Field (N/C)
  • k 9 x 109 N m2/C2
  • q Charge (C)
  • r distance from center of charge q (m)

29
iClicker
  • A point P is 0.50 meter from a point charge of
    5.0 X 10-8 coulomb. The intensity of the electric
    field at point P is most nearly
  • (A) 2.5 x 10-8 N/C
  • (B) 2.5 x 101 N/C
  • (C) 9.0 x 102 N/ C
  • (D) 1.8 x 103 N/C
  • (E) 7.5 x 108 N/C

30
iClicker
  • Charges Q and - 4Q are situated as shown above.
    The net electric field is zero nearest which
    point?
  • (A) A
  • (B) B
  • (C) C
  • (D) D
  • (E) E

31
Superposition of Fields
  • When more than one charge contributes to the
    electric field, the resultant electric field is
    the vector sum of the electric fields produced by
    the various charges.
  • Again, as with force vectors, this is referred to
    as superposition.

32
iClicker
  • The diagram above shows an isolated, positive
    charge Q. Point (B) is twice as far away from Q
    as point A. The ratio of the electric field
    strength at point A to the electric field
    strength at point B is
  • (A) 8 to 1
  • (B) 4 to 1
  • (C) 2 to 1
  • (D) 1 to 1
  • (E) 1 to 2

33
Electric Field Lines
  • Electric field lines are NOT VECTORS, but may be
    used to derive the direction of electric field
    vectors at given points.
  • The resulting vector gives the direction of the
    electric force on a positive charge placed in the
    field.

34
Problem
  • A particle bearing -5.0 µC is placed at -2.0 cm,
    and a particle bearing 5.0 µC is placed at 2.0
    cm. What is the field at the origin?

35
iClicker
  • An electron is accelerated from rest for a time
    of 10-9 second by a uniform electric field that
    exerts a force of 8.0 x 10-15 Newton on the
    electron.
  • What is the magnitude of the electric field?
  • (A) 8.0 x 10-24 N/C
  • (B) 9.1 x 10-22 N/C
  • (C) 8.0 x 10-6 N/C
  • (D) 2.0 x 10-5 N/C
  • (E) 5.0 x 104 N/C

36
iClicker
  • An electron is accelerated from rest for a time
    of 10-9 second by a uniform electric field that
    exerts a force of 8.0 x 10-15 Newton on the
    electron.
  • The speed of the electron after it has
    accelerated for the 10-9 second is most nearly
  • (A) 101 m/s
  • (B) 103 m/s
  • (C) 105 m/s
  • (D) 107 m/s
  • (E) 109 m/s

37
Problem
  • A particle bearing 10.0 mC is placed at the
    origin, and a particle bearing 5.0 mC is placed
    at 1.0 m. Where is the field zero?

38
Electric Potential
39
Electric Potential Energy
  • Electrical potential energy is the energy
    contained in a configuration of charges.
  • Like all potential energies, when it goes up the
    configuration is less stable when it goes down,
    the configuration is more stable.
  • The unit is the Joule.

40
Electric Potential Energy
  • Electrical potential energy increases when
    charges are brought into less favorable
    configurations


-
-
-
41
Electric Potential Energy
  • Electrical potential energy decreases when
    charges are brought into more favorable
    configurations.




-
42
Work
  • Work must be done on the charge to increase the
    electric potential energy.

43
Electric Potential
  • Electric potential is hard to understand, but
    easy to measure.
  • We commonly call it voltage, and its unit is
    the Volt.
  • 1 V 1 J/C
  • Electric potential is easily related to both the
    electric potential energy, and to the electric
    field.

44
Electric Potential
  • The change in potential energy is directly
    related to the change in voltage.
  • ?U q?V
  • ? U change in electrical potential energy (J)
  • q charge moved (C)
  • ? V potential difference (V)
  • All charges will spontaneously go to lower
    potential energies if they are allowed to move.

45
Electric Potential
  • Since all charges try to decrease U, and ?U q
    ?V, this means that spontaneous movement of
    charges result in negative ?U.
  • V U / q
  • Positive charges like to DECREASE their potential
    (?V lt 0)
  • Negative charges like to INCREASE their
    potential. (?V gt 0)

46
Problem
  • A 3.0 µC charge is moved through a potential
    difference of 640 V. What is its potential energy
    change?

47
E-field Potential
  • The electric potential is related in a simple way
    to a uniform electric field.
  • ?V -Ed
  • ?V change in electrical potential (V)
  • E Constant electric field strength (N/C or V/m)
  • d distance moved (m)

48
Problem
  • An electric field is parallel to the x-axis. What
    is its magnitude and direction of the electric
    field if the potential difference between x 1.0
    m and x 2.5 m is found to be 900 V?

49
More Electric Field Stuff
50
iClicker
  • Two large, flat, parallel, conducting plates are
    0.04 m apart, as shown above. The lower plate is
    at a potential of 2 V with respect to ground.
    The upper plate is at a potential of 10 V with
    respect to ground. Point P is located 0.01 m
    above the lower plate. The electric potential at
    point P is
  • a. 10 V
  • b. 8 V
  • c. 6 V
  • d. 4 V
  • e. 2 V

51
iClicker
  • The electron volt is a measure of
  • (A) Charge
  • (B) Energy
  • (C) Impulse
  • (D) Momentum
  • (E) velocity

52
iClicker
  • A point P is 0.50 meter from a point charge of
    5.0 X 10-8 coulomb. The electric potential at
    point P is most nearly
  • (A) 2.5 x l0-8 V
  • (B) 2.5 x 101 V
  • (C) 9.0 x 102 V
  • (D) 1.8x 103 V
  • (E) 7.5x 103 V

53
iClicker
  • The figure above shows two particles, each with a
    charge of Q, that are located at the opposite
    corners of a square of side d. What is the
    direction of the net electric field at point P ?
  • (A) Up and to the Right
  • (B) Up and to the Left
  • (C) Down and to the Right
  • (D) Down and to the Left
  • (E) Down

54
Charge Location
  • Electric field lines are more dense near a sharp
    point, indicating the electric field is more
    intense in such regions.
  • All lightning rods take advantage of this by
    having a sharply pointed tip.
  • During an electrical storm, the electric field at
    the tip becomes so intense that charge is given
    off into the atmosphere, discharging the area
    near a house at a steady rate and preventing a
    sudden blast of lightning.

55
Excess Charges
  • Excess charges reside on the surface of a charged
    conductor.
  • If excess charges were found inside a conductor,
    they would repel one another until the charges
    were as far from each other as possible, thus the
    surface.

56
E-Field of a Charged Sphere
  • The electric field inside a conductor must be
    zero.


E0












57
Conductor in an E-Field
  • The electric field inside a conductor must be
    zero.

58
iClicker
  • A positive charge of 10-6 coulomb is placed on an
    insulated solid conducting sphere. Which of the
    following is true?
  • The charge resides uniformly throughout the
    sphere
  • (B) The electric field inside the sphere is
    constant in magnitude, but not zero.
  • (C) The electric field in the region surrounding
    the sphere increases with increasing distance
    from the sphere.
  • (D) An insulated metal object acquires a net
    positive charge when brought near to, but not in
    contact with, the sphere.
  • (E) When a second conducting sphere is connected
    by a conducting wire to the first sphere, charge
    is transferred until the electric potentials of
    the two spheres are equal.

59
Electric Potential Energy
60
iClicker
  • Of the following phenomena, which provides the
    best evidence that particles can have wave
    properties?
  • (A) The absorption of photons by electrons in an
    atom
  • (B) The alpha-decay of radioactive nuclei
  • (C) The interference pattern produced by neutrons
    incident on a crystal
  • (D) The production of x-rays by electrons
    striking a metal target
  • (E) The scattering of photons by electrons at
    rest

61
Conservation of Energy
  • In a conservative system, energy changes from one
    form of mechanical energy to another.
  • When only the conservative electrostatic force is
    involved, a charged particle released from rest
    in an electric field will move so as to lose
    potential energy and gain an equivalent amount of
    kinetic energy.
  • The change in electrical potential energy can be
    calculated by
  • ?U q?V.

62
Problem
  • If a proton is accelerated through a potential
    difference of -2,000 V, what is its change in
    potential energy?
  • How fast will this proton be moving if it started
    at rest?

63
iClicker
  • Two parallel conducting plates are connected to a
    constant voltage source. The magnitude of the
    electric field between the plates is 2,000 N/C.
    If the voltage is doubled and the distance
    between the plates is reduced to 1/5 the original
    distance, the magnitude of the new electric field
    is
  • (A) 800 N/C
  • (B) 1,600 N/C
  • (C) 2,400 N/C
  • (D) 5,000 N/C
  • (E) 20,000 N/C

64
Problem
  • A proton at rest is released in a uniform
    electric field. How fast is it moving after it
    travels through a potential difference of -1200
    V? How far has it moved?

65
Electric Potential Energy
  • Electric potential energy is a scalar, like all
    forms of energy.
  • U kq1q2/r
  • U electrical potential energy (J)
  • k 9 109 N m2 / C2
  • q1, q2 charges (C)
  • r distance between centers (m)
  • This formula only works for spherical charges or
    point charges.

66
Electric Potential
  • For a spherical or point charge, the electric
    potential can be calculated by the following
    formula
  • V kq/r
  • V potential (V)
  • k 9 109 N m2 / C2
  • q charge (C)
  • r distance from the charge (m)

67
Problem
  • How far must the point charges q1 7.22 µC and
    q2 -26.1 µC be separated for the electric
    potential energy of the system to be -126 J?

68
Problem
  • The electric potential 1.5 m from a point charge
    q is 2.8 x 104 V. What is the value of q?

69
iClicker
  • The hollow metal sphere shown above is positively
    charged. Point C is the center of the sphere and
    point P is any other point within the sphere.
    Which of the following is true of the electric
    field at these points?
  • a. It is zero at both points.
  • b. It is zero at C, but at P it is not zero and
    is directed inward.
  • c. It is zero at C, but at P it is not zero and
    is directed outward.
  • d. It is zero at P, but at C it is not zero.
  • e. It is not zero at either point.

70
E-Field and Potential
71
Electric Field and Potential
  • E - V / d
  • Two things about E and V
  • The electric field points in the direction of
    decreasing electric potential.
  • The electric field is always perpendicular to the
    equipotential surface.

72
E-Field and Potential
  • The electric field points in the direction of
    decreasing electric potential.

73
E-Field is Perpendicular
  • Zero work is done when a charge is moved
    perpendicular to an electric field
  • W Fd cos 0
  • If zero work is done, and V - W/q, then there
    is no change in potential.
  • Thus, the potential is constant in a direction
    perpendicular to the electric field.

74
Problem
  • Draw a negative point charge of -Q and its
    associated electric field.
  • Draw 4 equipotential surfaces such that ?V is the
    same between the surfaces, and draw them at the
    correct relative locations.
  • What do you observe about the spacing between the
    equipotential surfaces?
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