Title: Coulombs Law and Electric Fields
1Coulombs Lawand Electric Fields
Physics 102 Lecture 02
- Today we will
- get some practice using Coulombs Law
- learn the concept of an Electric Field
2Recall 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
3Three 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
4Three 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
5Three 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
5 m
F-7
4 m
6 m
Q7.0mC
Q-7.0 mC
14
6Three 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
5 m
F-7
4 m
6 m
Q7.0mC
Q-7.0 mC
14
7Example
Adding Vectors F7F-7
8Example
Adding Vectors F7F-7
- y components cancel
- x components
-
9Example
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
10Gravitational 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
11Gravitational 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
12Electric 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
13Charged 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
14Preflight 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
15ACT 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
16ComparisonElectric 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
17E 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
18E 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-7
5 m
4 m
6 m
Q7.0mC
Q-7.0 mC
32
19Adding 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
20Adding 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
21Preflight 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
22ACT 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
23Electric 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
24Rules 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
25Electric Field Lines
42
26ACT/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
27ACT/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
28ACT/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
29ACT E Field Lines
B
A
Compare the magnitude of the electric field at
point A and B 1) EAgtEB 2) EAEB 3) EAltEB
47
30E 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
31ACT/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
32Recap
- 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
33To 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!