1. © 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including on the World Wide Web) will destroy the integrity of the work and is not permitted. The work and materials from it should never be made available to students except by instructors using the accompanying text in their classes. All recipients of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of other instructors who rely on these materials. Lecture Outlines Chapter 15 College Physics, 6 th Edition Wilson / Buffa / Lou

2. Chapter 15 Electric Charge, Forces, and Fields

3. Units of Chapter 15 Electric Charge Electrostatic Charging Electric Force Electric Field Conductors and Electric Fields Gauss’s Law for Electric Fields: A Qualitative Approach

4. 15.1 Electric Charge Electric charge is a fundamental property of matter; electric charges may be positive or negative. The atom consists of a small positive nucleus surrounded by a negative electron cloud.

5. 15.1 Electric Charge Like charges repel; unlike charges attract.

6. 15.1 Electric Charge SI unit of charge: the coulomb, C. All charges are integer multiples of the charge on the electron:

7. 15.1 Electric Charge Charge is conserved: The net charge of an isolated system remains constant.

8. 15.2 Electrostatic Charging Conductors transmit charges readily. Semiconductors are intermediate; their conductivity can depend on impurities and can be manipulated by external voltages. Insulators do not transmit charge at all.

9. 15.2 Electrostatic Charging An electroscope may be used to determine if an object is electrically charged.

10. 15.2 Electrostatic Charging Charging by friction: This is the process by which you get “charged up” walking across the carpet in the winter. It is also the process that creates “static cling” in your laundry, and makes it possible for you to rub a balloon on your hair and then stick the balloon to the wall.

11. 15.2 Electrostatic Charging An electroscope can be given a net charge by conduction—when it is touched with a charged object, the excess charges flow freely onto the electroscope.

12. 15.2 Electrostatic Charging An electroscope may also be charged by induction, if there is a way of grounding it while charge is being induced.

13. 15.2 Electrostatic Charging Charge may also be moved within an object—without changing its net charge—through a process called polarization.

14. 15.3 Electric Force The force exerted by one charged particle on another is given by:

15. 15.3 Electric Force If there are multiple point charges, the force vectors must be added to get the net force.

16. 15.4 Electric Field Definition of the electric field: The direction of the field is the direction the force would be on a positive charge.

17. 15.4 Electric Field Charges create electric fields, and these fields in turn exert electric forces on other charges. Electric field of a point charge:

18. 15.4 Electric Field For multiple charges, the total electric field is found using the superposition principle: For a configuration of charges, the total, or net, electric field at any point is the vector sum of the electric fields due to the individual charges.

19. 15.4 Electric Field It is convenient to represent the electric field using electric field lines, or lines of force. These lines are drawn so the field is tangent to the line at every point.

20. 15.4 Electric Field Rules for drawing electric field lines: 1. Closer lines mean a stronger field. 2. The field is tangent to the lines at every point. 3. Field lines start on positive charges and end on negative charges. 4. The number of lines entering or leaving a charge is proportional to the magnitude of the charge. 5. Field lines never cross.

21. 15.4 Electric Field Electric field lines of a dipole:

22. 15.4 Electric Field Electric field lines due to very large parallel plates:

23. 15.4 Electric Field Electric field lines due to like charges: (a) equal charges; (b) unequal charges.

24. 15.5 Conductors and Electric Fields Electric charges are free to move within a conductor; therefore, there cannot be a static field within the conductor: The electric field is zero inside a charged conductor. Excess charges on a conductor will repel each other, and will wind up being as far apart as possible. Any excess charge on an isolated conductor resides entirely on the surface of the conductor.

25. 15.5 Conductors and Electric Fields There cannot be any component of the electric field parallel to the surface of a conductor; otherwise charges would move. The electric field at the surface of a charged conductor is perpendicular to the surface.

26. 15.5 Conductors and Electric Fields The force from neighboring charges is less when the curvature of the surface is large: Excess charge tends to accumulate at sharp points, or locations of highest curvature, on charged conductors. As a result, the electric field is greatest at such locations.

27. 15.6 Gauss’s Law for Electric Fields: A Qualitative Approach A surface, called a Gaussian surface, that completely surrounds a point charge intercepts the same number of field lines regardless of its shape. For a positive charge, the lines exit the surface; for a negative one they enter it.

28. 15.6 Gauss’s Law for Electric Fields: A Qualitative Approach If a greater amount of charge is enclosed, more field lines cross the surface.

29. 15.6 Gauss’s Law for Electric Fields: A Qualitative Approach Here, surface 1 surrounds the positive charge and has lines exiting it. Surface 2 surrounds the negative charge and has lines entering it. Surface 3 does not enclose any charge, and the same number of lines exit as enter. Surface 4 encloses both charges; as they are equal in magnitude, the same number of lines exit the surface as enter it.

30. 15.6 Gauss’s Law for Electric Fields: A Qualitative Approach The underlying physical principle of Gauss’s law: The net number of electric field lines passing through an imaginary closed surface is proportional to the amount of net charge enclosed within that surface. This can be used to show that excess charge on a conductor must reside on the surface.

31. Summary of Chapter 15 Like charges repel; unlike charges attract. Charge is conserved. Electrons move freely inside conductors, but not inside insulators. Objects may be charged electrostatically by friction, conduction, or induction. Polarization is the separation of positive and negative charge within an object.

32. Summary of Chapter 15 Coulomb’s law: The electric field, a vector, is the force per unit charge. Electric fields from multiple charges add by superposition. Electric field lines are used to represent the electric field. A conductor has zero electric field inside and has all excess charge on its surface.

33. Summary of Chapter 15 The electric field is always perpendicular to the surface of a conductor. The charge density and electric field are greatest on a conductor where the curvature is largest.