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Coulombs Law and Electric Fields

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Recall Coulomb's Law. Magnitude of the force between charges q1 and q2 separated a distance r: ... g = GM/r2. Force on m due to gravitational field. F = mg ... – PowerPoint PPT presentation

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Title: Coulombs Law and Electric Fields


1
Coulombs Lawand Electric Fields
Physics 102 Lecture 02
  • Today we will
  • get some practice using Coulombs Law
  • learn the concept of an Electric Field

2
Recall Coulombs Law
  • Magnitude of the force between charges q1 and q2
    separated a distance r
  • F k q1q2/r2 k 9x109 Nm2/C2
  • Force is
  • attractive if q1 and q2 have opposite sign
  • repulsive if q1 and q2 have same sign
  • Units
  • qs have units of Coulombs (C)
  • charge on proton is 1.6 x 10-19 C
  • r has units of m
  • F has units of N

5
3
Three Charges
Example
  • Calculate force on 2mC charge due to other two
    charges
  • Calculate force from 7mC charge
  • Calculate force from 7mC charge
  • Add (VECTORS!)

Q2.0mC
4 m
6 m
Q7.0mC
Q-7.0 mC
10
4
Three Charges
Example
  • Calculate force on 2mC charge due to other two
    charges
  • Calculate force from 7mC charge
  • Calculate force from 7mC charge
  • Add (VECTORS!)

Q2.0mC
4 m
6 m
Q7.0mC
Q-7.0 mC
10
5
Three Charges
Example
  • Calculate force on 2mC charge due to other two
    charges
  • Calculate force from 7mC charge
  • Calculate force from 7mC charge
  • Add (VECTORS!)

F7
Q2.0mC
  • F k q1q2/r2

5 m
F-7
4 m
6 m
Q7.0mC
Q-7.0 mC
14
6
Three Charges
Example
  • Calculate force on 2mC charge due to other two
    charges
  • Calculate force from 7mC charge
  • Calculate force from 7mC charge
  • Add (VECTORS!)

F7
Q2.0mC
  • F k q1q2/r2

5 m
F-7
4 m
6 m
Q7.0mC
Q-7.0 mC
14
7
Example
Adding Vectors F7F-7
8
Example
Adding Vectors F7F-7
  • y components cancel
  • x components

9
Example
Adding Vectors F7F-7
  • y components cancel
  • x components
  • F F7,x F-7,x
  • F7,x (3/5)F7
  • F-7,x (3/5)F-7
  • F (3/5)(55)x10-3 N6 x 10-3 N

You will have lots of opportunity to practice
this in homework and discussion
10
Gravitational Field An Analogy to the Electric
Field
  • Force on m due to M
  • F GMm/r2 GM/r2m
  • Gravitational field due to M
  • g GM/r2
  • Force on m due to gravitational field
  • F mg
  • Identical to F GMm/r2

m
M
21
11
Gravitational Field An Analogy to the Electric
Field
q
  • Force on q due to Q
  • F kQq/r2 kQ/r2q
  • Electric field due to Q
  • E kQ/r2
  • Force on q due to electric field
  • F qE
  • Identical to F kQq/r2

Q
21
12
Electric vs. Gravitational Fields
  • Charges produces electric fields
  • Just like masses produce gravitational fields
  • Electric fields exert forces on charges
  • Just like gravitational fields exert forces on
    masses
  • Electric fields and gravitational fields are both
    vectors
  • Gravitational field due to a mass always points
    towards that mass (e.g., toward the center of
    Earth)
  • Electric field due to a charge Q points
  • towards Q if Qlt0
  • away from Q if Qgt0

13
Charged particles create electric fields.
  • Direction points away from charge and toward
    charge.
  • Magnitude given by E ? kq/r2
  • Units N/C (Force/charge)

Example
E
E (9?109)(1.6?10-19)/(10-10)2 N/C 1.4?1011 N/C
(to the right)
21
14
Preflight 2.3
  • What is the direction of the electric field at
    point B?
  • Left
  • Right
  • Zero

72 16 9
it is closer to the negative charge, and the
field lines point toward negative charges .
B only has the charge from the negative which is
pushing away from itself .
electric fields of equal magnitudes but opposite
directions are present due to the positive and
negative charges .
Since charges have equal magnitude, and point B
is closer to the negative charge net electric
field is to the left
y
A
B
x
23
15
ACT E Field
  • What is the direction of the electric field at
    point C?
  • Left
  • Right
  • Zero

Red is negative Blue is positive
Away from positive charge (right)
Towards negative charge (right)
Net E field is to right.
y
C
x
25
16
ComparisonElectric Force vs. Electric Field
  • Electric Force (F) - the actual force felt by a
    charge at some location.
  • Electric Field (E) - found for a location only
    tells what the electric force would be if a
    charge were located there
  • F Eq
  • Both are vectors, with magnitude and direction.
    Add x y components. Direction determines sign.

26
17
E Field from 2 Charges
Example
  • Calculate electric field at point A due to
    charges
  • Calculate E from 7mC charge
  • Calculate E from 7mC charge
  • Add (VECTORS!)

A
Note this is similar to my earlier example.
4 m
You will have lots of opportunity to practice
this in homework and discussion
6 m
Q7.0mC
Q-7.0 mC
28
18
E Field from 2 Charges
Example
  • Calculate electric field at point A due to
    charges
  • Calculate E from 7mC charge
  • Calculate E from 7mC charge
  • Add vectors

E7
  • E k q/r2

E-7
5 m
4 m
6 m
Q7.0mC
Q-7.0 mC
32
19
Adding Vectors E7E3
Example
  • Decompose into x and y components.
  • Add components.
  • Note that y components cancel

E7
Etotal
5m
4 m
E-7
3m
6 m
Q7.0mC
Q-3.5 mC
35
20
Adding Vectors E7E3
Example
  • Decompose into x and y components.
  • Add components.
  • Note that y components cancel

E7
Etotal
5m
4 m
E-7
3m
6 m
Q7.0mC
Q-3.5 mC
35
21
Preflight 2.2
  • What is the direction of the electric field at
    point A?
  • Up
  • Down
  • Left
  • Right
  • Zero

Red is negative Blue is positive
6 8 3 58 25
y
A
B
x
37
22
ACT E Field II
  • What is the direction of the electric field at
    point A, if the two positive charges have equal
    magnitude?
  • Up
  • Down
  • Right
  • Left
  • Zero

Red is negative Blue is positive
y
A
B
x
39
23
Electric Field Lines
  • Closeness of lines shows field strength
  • - lines never cross
  • lines at surface ? Q
  • Arrow gives direction of E
  • - Start on , end on -

42
24
Rules for Electric Field Lines
  • They start only on charges and end only on
    charges
  • lines starting or stopping on a charge is
    proportional to the magnitude of the charge
  • Tangent to field lines gives direction of field
    at that point
  • Field lines can never cross
  • Density of field lines is proportional to the
    strength of the field

25
Electric Field Lines
42
26
ACT/Preflight 2.5
Charge A is 1) positive 2) negative 3) unknown
Field lines start on positive charge, end on
negative.
93 4 3
44
27
ACT/Preflight 2.6
X
A
B
Y
Compare the ratio of charges QA/ QB 1) QA 0.5QB
2) QA QB 3) QA 2 QB
lines proportional to Q
12 9 63
45
28
ACT/Preflight 2.8
The electric field is stronger when the lines
are located closer to one another.
The magnitude of the electric field at point X is
greater than at point Y 1) True 2) False
Density of field lines gives E
14 86
46
29
ACT E Field Lines
B
A
Compare the magnitude of the electric field at
point A and B 1) EAgtEB 2) EAEB 3) EAltEB
47
30
E inside of conductor
  • Conductor ? electrons free to move
  • Electrons feels electric force - will move until
    they feel no more force (F0)
  • FEq if F0 then E0
  • E0 inside a conductor (Always!)

48
31
ACT/Preflight 2.10
"Charge A" is actually a small, charged metal
ball (a conductor). The magnitude of the electric
field inside the ball is (1) Negative (2)
Zero (3) Positive
9 74
18
50
32
Recap
  • E Field has magnitude and direction
  • E?F/q
  • Calculate just like Coulombs law
  • Careful when adding vectors
  • Electric Field Lines
  • Density gives strength ( proportional to
    charge.)
  • Arrow gives direction (Start end on -)
  • Conductors
  • Electrons free to move ? E0

33
To Do
  • Read Sections 17.1-17.3
  • Extra problems from book Ch 16
  • Concepts 9-15
  • Problems 11, 15, 23, 27, 29, 39
  • Do your preflight by 600 AM Wednesday.

Have a great weekend. No classes Monday. See
you next Wednesday!
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