1. Test on Electricity and Magnetism on Feb 20 and Feb 21
Static Electricity
Test on Electricity and Magnetism on Feb 20 and Feb 21

2. Electric Charges Negative charge comes from extra electrons
Positive charge comes from lack of electrons
Law of Conservation of Electric Charge
Net amount of charge produced is zero.
Like charges repel
Opposite charges attract
Charge can be transferred from one object to another
e = charge of one electron = x C

3. Insulators and Conductors
Conductors allow electrons to pass through them
Insulators prevent electrons from passing through them
Semi-conductors have characteristics of both
Free Electrons

4. Conduction
When a charged object touches a conductor, some of the charge will be transferred to the conductor. Now both objects will have the same charge and the objects will be repelled.
This charging is permanent.
When the charged object is removed, both objects will retain their charge.

5. Induction
A charged object is brought close to a conductor without touching it. The charges inside the conductor separate so that likes repel and opposites attract. The objects will be attracted to each other.
This charging is only temporary.
When the charged object is removed, the conductor returns to normal.

6. The Electroscope
Homework – research and build an electroscope. Make sure you know how it works and what is happening inside of it. Bring it to class in on Friday.

7. Electric Force
Every electric charge produces a field force that attracts or repels other charges.
The electric force obeys the inverse square law.
The force of attraction/repulsion between charges is called Coulumb’s Law
F = kQ1Q2/r2
k = 9 x 109 Nm2/C2

8. Electric Force This equation applies for point charges only,
And only for objects at rest.
If there are two charges, the force on charge A is equal to the force on charge B.
If there are more than two charges, then the forces add together.

9. How do you feel about some…
Examples?!

10. Electric Field
The electric force is a field force (force that can act without touching) therefore it generates a field around it. Anything that comes into the field will feel its force.
Every charged particle creates its own electric field and multiple fields may exist.
The field obeys the inverse square law.
E = kQ/r2 = F/Q2

11. How do you feel about some more…
Examples?!

12. Electric Field
The electric field can be shown by drawing lines that show the direction a positively charged particle would travel.
The electric field and electric force are vectors so they can be added together. Pay attention to sign.

13. Electric Fields
Dipoles

14. Electric Field Lines
The field lines indicate the direction of the electric field
The lines are drawn so that the magnitude of the field is proportional to the number of lines drawn. Closer lines = stronger field
Electric field lines start on positive charges and end on negative ones. The # starting or ending is pro. to the mag. of the charge

15. Electric Fields
Strength of Field

16. Conductors in a Field The electric field inside a conductor is zero.
The electric field is always perpendicular to the surface outside of a conductor.

17. Parallel Plates This setup creates a scenario similar to gravity.
A charged particle moving through this setup would feel a pull (+ downward, - upward)
The result is a projectile motion problem with electric force instead of gravity.
F = ma
qE = ma  a = qE/m

18. Electric Potential Conservation of energy Electric potential
Potential energy per unit charge
Parallel plates
Work-Energy Theorem
The amount of work required to move a charge in an electric field is equal to a change in the kinetic (or potential) energy

19. Electric Potential
The work done to move that charge depends on the magnitude of that charge.
Positive work is in the direction of motion. Negative work is done in the direction opposite motion.
Electric Potential (V)
V = PE/q
PEelectric = kQ1Q2/r
V = kq/r

20. Electric Potential Difference
The difference in electric potential as you move from point A to point B
Measured in volts
V= - Work/q = ΔPE/q
Electric Potential Difference is like Gravitational Potential Energy in the sense that you may choose a place where the electric potential is zero to make calculations easier.

21. Electric Potential and Electric Field
Vba = Ed
Places where the electric potential are the same are shown by equipotential lines
Drawn perpendicular to the electric field lines

22. Capacitors Device that can store electric charge
Consists of two conducting surfaces not in contact
One surface acquires a positive charge, the other surface acquires a negative charge
Eventually the surfaces will become “full” and charge will leak.
A dielectric separates the two surfaces

23. Capacitors Parallel Plate Capacitors C = capacitance C = ε0A/d
ε0= 1/4πk