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Electric Forces and Fields

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Electric Forces and Fields Chapter 20 Adding Electric forces in 2 dimension Next add the components of the net force F3x =F(1on3)x + F(2on 3)x = -1.9 X 10-3 N -1.9 x ... – PowerPoint PPT presentation

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Title: Electric Forces and Fields


1
Electric Forces and Fields
  • Chapter 20

2
Charges and ForcesExperiment 1
  • Nothing happens
  • The objects are neutral

3
Charges and ForcesExperiment 2
  • The two rods repel each other
  • A rubbed rod is charged
  • Long range repulsive force

4
Charges and ForcesExperiment 3
  • These rods attract each other
  • Positive and negative charges

5
Charges and ForcesExperiment 4
  • When two rods are rubbed more vigorously the
    strength of the forces is greater
  • The strength of the
  • charges decreases
  • as the distance
  • between the rods
  • increases

6
Charges and ForcesExperiment 5
  • Rub a plastic rod with wool
  • The rod is weakly attracted to the wool
  • The rod is repelled by a piece of silk that has
    been used to
  • rub glass

7
Charges and ForcesExperiment 6
  • Charged plastic rod held over paper
  • The neutral paper is attracted to the rod
  • A charged glass rod attracts the paper
  • A neutral rod has no effect on the paper

8
Charge Separation
  • A charged object can induce a charge separation
    on an uncharged object that can lead to an
    attractive force. http//phet.colorado.edu/simulat
    ions/sims.php?simBalloons_and_Static_Electricity

9
Insulators and ConductorsHow does charge move on
different materials?
  • Charge a plastic rod by rubbing it with wool
  • Touch a neutral metal sphere
  • The sphere acquires the charge of the rod

10
Insulators and ConductorsHow does charge move on
different materials?
  • The metal sphere that is touched by the charged
    plastic rod will pick up small pieces of paper
    (it is charged)
  • The other sphere will not (it remains neutral)

11
Insulators and ConductorsHow does charge move on
different materials?
  • Touch one sphere with a charged plastic rod
  • Both spheres will attract small bits of paper
    (they are charged)

12
Transfer of Charge
  • Charge can be transferred from one object to
    another when the objects touch.
  • Removing charge from an object is called
    discharging
  • Charge is conserved (it cant be created or
    destroyed

13
Transfer of charge
  • Conductors material through or along which
    charge easily moves
  • Metal
  • Insulators materials on or in which charges
    remain immobile
  • Glass and plastic
  • Both insulators and conductors can be charged.
    They differ in the mobility of the charge

14
Charge diagram
  • An insulating rod is charged by rubbing
  • Charges on the insulator rod dont move

15
Charge diagram
  • Charges in a conductor are free to move

16
Electrostatic Equilibrium
  • The charges on an isolated conductor are in
    static equilibrium other than the brief interval
    when the charges are adjusting
  • The charges are at rest
  • No net force on any charge

17
ElectroscopeCharge polarization
  • The charges move around but
  • Charge is conserved
  • Slight separation of
  • the positive and
  • negative charge in a
  • neutral object

18
Polarization Force
  • The polarization force arises because the charges
    in the metal are separated NOT because the rod
    and metal are oppositely charges

19
Fundamental Charge
  • Charge is represented by the symbol q
  • The SI unit of charge is the coulomb (C)
  • Protons and electrons have the same amount of
    charge but opposite signs
  • The fundamental or elementary charge (e) is the
    magnitude of the charge of a proton or electron
  • e 1.60 X 10-19 C

20
Fundamental Charge
  • Charge is conserved
  • The total amount of charge remains constant

21
Coulombs Law
  • Electric force increases for objects with more
    charge and decreases as charged objects are moved
    farther apart.

22
Coulombs Law Equation
  • K is the electrostatic constant
  • K 8.99 x109 N m2/C2
  • C are units of electric charge called coulombs
  • r is the distance the charges are apart

23
Direction of forces
  • The forces are directed along the line joining
    the two particles
  • The forces are repulsive for two like charges
  • The forces are attractive for two opposite
    charges
  • These forces are an action/reaction pair equal in
    magnitude but opposite in direction.

24
Forces are Vectors
  • Electric forces are represented by vectors
  • Like other forces they can be superimposed
  • If multiple charges are acting on charge j, the
    net electric force on charge j is the sum of all
    the individual forces due to each charge.
  • Fnet F1onj F 2on j F3onj

25
Adding Electric Forces in 1 dimension
  • Example 20.1
  • A. Two 10nCcharged particles are 2.0 cm apart on
    the x-axis. What is the net force on a
  • 1.0 nC charge midway between them?
  • Fnet F1on3 F2on3
  • Fnet 0
  • q1 and q2 exert repulsive forces on q3. Equal in
    magnitude, opposite in direction

26
Adding Electric Forces in 1 dimension
  • 20.1 b. What is the net force if the charged
    particle on the right is replaced by a -10 nC
    charge?
  • Forces are equal in magnitude and direction
  • Fnet 2F1on3

27
Adding Electric Forces in 1 dimension
  • 20.1 B. The magnitude is given by Coulombs Law
  • F1on3 9.0 x 10-4 N
  • Fnet 2(F1on3)
  • 1.8 X 10-3 N to the right

28
Adding Electric forces in 2 dimension
  • Example 20.2
  • Three charges particle with q1 -50nC, q2
    50nC, and q3 30nC are placed as shown. What
    is the net force on charge q3 due to the other 2
    charges

29
Adding Electric forces in 2 dimension
  • Define a coordinate system with q3 at the origin.
  • Draw the forces on the charge q3 with direction
    determined by the signs of the charges.

30
Adding Electric forces in 2 dimension
31
Adding Electric forces in 2 dimension
  • Determine the net force on charge q3 using
    Coulombs law
  • 2.7 x 10-3 N

32
Adding Electric forces in 2 dimension
  • Determine the net force on charge q3 using
    Coulombs law
  • Magnitude and distance are the same for F2on3
  • 2.7 x 10-3 N

33
Adding Electric forces in 2 dimension
  • Compute values for the componentsusing trig.
  • (F1on3)x -1.9x10-3 N
  • (F1on3)y -1.9x10-3 N
  • (F2on3)x -1.9x10-3 N
  • (F2on3)y -1.9x10-3 N

34
Adding Electric forces in 2 dimension
  • Next add the components of the net force
  • F3x F(1on3)x F(2on 3)x
  • -1.9 X 10-3 N -1.9 x 10-3 N 3.8 x10-3N
  • F3y F(1on3)y F(2on3)y
  • 1.9 X 10-3 N -1.9 x 10-3 N 0
  • Net force is F3
  • 3.8 x10-3N, -x direction

35
The Electric Field
  • Grass seed in a pan of oil
  • When charged spheres
  • ( and -) touch the surface,
  • the grass seeds line up
  • in a regular pattern.
  • The pattern suggests that some kind of electric
    influence fills the space around the charges.
  • This alteration of space could be the mechanism
    by which the long range Coulombs Law force is
    exerted.

36
The Field Model
  • The alteration of space around charge is the
    agent that exerts a force on charge B
  • This alteration of space is called a field
  • The charges make an alteration everywhere in
    space
  • Other charges then respond to those alteration at
    their position

37
The Field Model
38
The Field Model
  • The field model applies to many branches of
    science
  • Electric field-alteration of space around a
    charge
  • Gravitational Field-alteration of space around a
    mass
  • Magnetic Field-alteration of space around a magnet

39
Field Model
  • Source Charges alter the space around them by
    creating an electric field E.
  • A separate charge in the electric field then
    experiences a force F exerted by the field

40
Electric Field Diagram
41
Electric Field Diagram
42
Electric Field Diagram
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