1. Chapter 16 Electric Charge and Electric Field © 2008 Giancoli, PHYSICS,6/E © 2004. Electronically reproduced by permission of Pearson Education, Inc., Upper Saddle River, New Jersey

2. Ch162 Structure of the atom (protons, neutrons and electrons) Nucleus contains protons and neutrons Protons have positive charge, neutrons are neutral Mass of proton ≈ mass of neutron Mass of proton (and neutron)  1800x mass of electron Electrons have negative charge and are attracted to nucleus Charge of electron is equal in magnitude to that of proton Normal atom is neutral Ion is atom that has gained or lost one or more electrons

3. Ch163 Conductors and Insulators Conductor: metal atoms in solids have one or more “free” electrons per atom which move freely through the material Insulator: no free electrons so it will not conduct electricity

4. Ch164 Static Electricity Static Electricity: Rubbing certain materials together can separate electrons from their atoms Removing electrons from a material makes it positive In solids, it is always the free electrons that move Electrical charge on the plastic rod induces a separation of charge in scraps of paper and thus attracts them.

5. Ch165 Induced Charge (a) If you bring a + charge near a conductor, it will attract electrons to it leaving the other half of the metal positive. (b) If they touch, then electrons move to the positively charged object, leaving the conductor positively charged.

6. Ch166 Coulomb’s Law Forces are equal in magnitude but opposite in direction For spherical charges, r is the center to center distance This equation gives the magnitude of the force--you have to figure the direction from the signs of the charges

7. Ch167 Coulomb’s Law k  9.0  10 9 N·m 2 / C 2 C is Coulomb -- the unit of charge e = 1.60x10 -19 C electronic charge (positive)

8. Ch168 Coulomb’s Law

9. Ch169 Example 1. Particles of charge Q 1 = +5.00  C, Q 2 = -6.0  C and Q 3 = +8.0  C are placed in a line separated by 0.40 m between each pair. Calculate the force on Q 2. + Q1Q1 _ Q2Q2 + Q3Q3 This is the magnitude, we get direction from charges. Force is directed to the right.

10. Ch1610 Example 2. Particles of charge Q 1 = +5.00  C, Q 2 = -6.00  C and Q 3 = +8.00  C are placed on the corners of a square of side 0.400 m as shown below. Calculate the force on Q 2 (Magnitude and direction). + Q1Q1 _ Q2Q2 +Q3Q3 Note that the charges and distances are the same as in Example 1, so we do not need to use Coulombs Law again. 

11. Ch1611 The Electric Field Graphical representation of electrical forces Electrical force “acts at a distance” like gravity Electric field E surrounds every charge We investigate the field with a small positive charge called a “test charge” q The field is given by:

12. Ch1612 The Electric Field Units are N/C E is a vector = direction of force experienced by positive test charge The magnitude of q is so small that it does not disturb the charges that cause the field To plot the field, move the test charge around the charges that cause the field Since q is positive the field points away from a + charge and towards a - charge

13. Ch1613 Field of a Point Charge Q This is the field created by a point charge or a spherical charge distribution Q

14. Ch1614 Electric Field is a Vector Field thus points toward a negative charge and away from a positive charge Since test charge is positive, the direction of the electric field is the direction of the force felt by a positive charge If there are two or more charges creating the field then the field at any point is the vector sum of the fields created by each of the charges The test charge does not contribute to the field and it is too weak to cause any of the charges creating the field to move.

15. Ch1615 Example 3A. A +100  C point charge is separated from a -50  C charge by a distance of 0.50 m as shown below. (A) First calculate the electric field at midway between the two charges. (B) Find the force on an electron that is placed at this point and then calculate the acceleration when it is released. E1E1 E2E2 + Q1Q1 _ Q2Q2

16. Ch1616 Example 3B. A +100  C point charge is separated from a -50  C charge by a distance of 0.50 m as shown below. (A) First calculate the electric field at midway between the two charges. (B) Find the force on an electron that is placed at this point and then calculate the acceleration when it is released. + Q1Q1 _ Q2Q2 In part A we found that E = 2.1x10 7 N/C and is directed to the right. ( to left )

17. Ch1617 Example 4. A +100  C point charge is separated from a -50  C charge by a distance of 0.50 m as shown below. Sketch the electric field at the point x as shown. + Q1Q1 _ Q2Q2

18. Ch1618 Electric Field Lines Graphical way of showing the electric field. You have seen graphical representations of the earth’s magnetic field-the electric field maps are similar. Sometimes called lines of force. Arrow on field line gives direction of force. The closer together the lines of force are, the stronger the electric field. Electric field lines are directed out from positive charges (a) and in toward negative charges (b).

19. Ch1619 Electric Field of Point Charges

20. Ch1620 Electric Field of Point Charges

21. Ch1621 Electric Field of Parallel Plates

22. Ch1622 Electric Fields and Conductors In the static situation, the field outside the conductor is perpendicular to the surface of the conductor if the field had a component parallel to the surface, it would cause the electrons in the conductor to move until there was only a perpendicular component.

23. Ch1623 Electric Fields and Conductors If a conductor is placed in an electric field, the electrons will rearrange themselves until the field inside the conductor is zero The field inside a hollow conductor shell is zero (Fig 16-33) This makes a metal car a relatively safe place in an electrical storm.