Title: Electric Forces and Fields
1Electric Forces and Fields
2Charges and ForcesExperiment 1
- Nothing happens
- The objects are neutral
3Charges and ForcesExperiment 2
- The two rods repel each other
- A rubbed rod is charged
- Long range repulsive force
4Charges and ForcesExperiment 3
- These rods attract each other
- Positive and negative charges
5Charges 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
6Charges 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
7Charges 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
8Charge 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
9Insulators 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
10Insulators 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)
11Insulators 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)
12Transfer 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
13Transfer 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
14Charge diagram
- An insulating rod is charged by rubbing
- Charges on the insulator rod dont move
15Charge diagram
- Charges in a conductor are free to move
16Electrostatic 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
17ElectroscopeCharge polarization
- The charges move around but
- Charge is conserved
- Slight separation of
- the positive and
- negative charge in a
- neutral object
18Polarization Force
- The polarization force arises because the charges
in the metal are separated NOT because the rod
and metal are oppositely charges
19Fundamental 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
20Fundamental Charge
- Charge is conserved
- The total amount of charge remains constant
21Coulombs Law
- Electric force increases for objects with more
charge and decreases as charged objects are moved
farther apart.
22Coulombs 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
23Direction 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.
24Forces 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
25Adding 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
26Adding 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
27Adding 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
28Adding 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
29Adding 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.
30Adding Electric forces in 2 dimension
31Adding Electric forces in 2 dimension
- Determine the net force on charge q3 using
Coulombs law - 2.7 x 10-3 N
32Adding 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
33Adding 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
34Adding 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
35The 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.
36The 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
37The Field Model
38The 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
39Field 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
40Electric Field Diagram
41Electric Field Diagram
42Electric Field Diagram