1. Chapter 21 Electric Field 1

2. Chapter 21.1 The Electric Field Define an electric field Solve problems relating to charge, electric fields, and forces. Diagram electric field Energy and Electric potential Storing charges: Capacitor

3. The Electric Field Definition of the electric field: Here, q 0 is a “test charge” – it serves to allow the electric force to be measured, but is not large enough to create a significant force on any other charges.

4. The Electric Field If we know the electric field, we can calculate the force on any charge: The direction of the force depends on the sign of the charge : for a positive charge – the same direction for a negative - opposite

5. Example An electric field is measured using a positive test charge of 3.0 μC. It experiences a force of 0.24 N at an angle of 15 degree north of east. What are the magnitude and direction of the electric field strength at the location of the test charge?

6. The Electric Field The electric field of a point charge points radially away from a positive charge and towards a negative one.

7. The Electric Field Just as electric forces can be superposed, electric fields can as well.

8. Electric Field Lines Electric field line is the lines to represent the actual field in the space around charge. EF lines: 1.Start at positive charges or infinity 2.End at negative charges or infinity 3.Are more dense where the field is stronger. 4.Always perpendicular to the surface of a conductor. 5.EF is stronger where the surface is more sharply curved.

9. Electric Field Lines The charge on the right is twice the magnitude of the charge on the left (and opposite in sign), so there are twice as many field lines, and they point towards the charge rather than away from it.

10. Electric Field Lines Combinations of charges. Note that, while the lines are less dense where the field is weaker, the field is not necessarily zero where there are no lines. In fact, there is only one point within the figures below where the field is zero – can you find it?

11. Electric Field Lines

12. Shielding and Charge by Induction When electric charges are at rest, the electric field within a conductor is zero.

13. Chapter 21.2 Electric Potential and Electric Potential Energy

14. Electric Potential Electric Potential Difference Electric Potential Energy Equipotential Surfaces and the Electric Field

15. Electric potential energy and Electric potential EPE is the negative work to move an electric charge to an electric field. In electricity, it is more convenient to use the EPE per unit charge, just called Electric potential or voltage.

16. Electric Potential Energy and the Electric Potential The electric field is related to how fast the potential is changing:

17. The Electric Potential of Point Charges The difference in potential energy (EPD) between points A and B is the ratio of the work needed to move a charge to the strength of that charge

18. The Electric Potential of Point Charges Therefore, the electric potential of a point charge is:

19. Equipotential Surfaces and the Electric Field Equipotential surfaces are those on which the electric potential is constant. The electric field is perpendicular to the equipotential surfaces.

20. Equipotential Surfaces and the Electric Field For two point charges:

21. P 571 # 16-25 even

22. Capacitors and Dielectrics A capacitor is two conducting plates separated by a finite distance:

23. The capacitance relates the charge to the potential difference: Capacitors and Dielectrics

24. A simple capacitor is the parallel-plate capacitor. It consists of two plates of area A separated by a distance d. The general properties of a parallel-plate capacitor –

25. Capacitors and Dielectrics A dielectric is an insulator; when placed between the plates of a capacitor it gives a lower potential difference with the same charge, due to the polarization of the material. This increases the capacitance.

26. Capacitors and Dielectrics The dielectric constant is a property of the material; here are some examples:

27. P 578, # 30-34 Do prelab Page 580 -Testable question -Hypothesis -Data table

28. Summary A spherical charge distribution behaves from the outside as though the total charge were at its center Electric field is the force per unit charge; for a point charge: Electric fields created by several charges add as vectors

29. Summary Electric field lines help visualize the electric field Field lines point in the direction of the field; start on + charges or infinity; end on – charges or infinity; are denser where E is greater Parallel-plate capacitor: two oppositely charged, conducting parallel plates Excess charge on a conductor is on the surface Electric field within a conductor is zero (if charges are static)