1. The problem solving session will be Wednesdays from 12:30 – 2:30 (or until there is nobody left asking questions) in FN 2.212

2. Torque on the electric dipole Electric field is uniform in space Net Force is zero Net Torque is not zero (torque is a vector) Stable and unstable equilibrium (electric dipole moment from “-” to “+”)

3. Charge #1 Charge #2 Charge #3 +q+q +q+q –q–q x y A. clockwise. B. counterclockwise. C. zero. D. not enough information given to decide Three point charges lie at the vertices of an equilateral triangle as shown. Charges #2 and #3 make up an electric dipole. The net electric torque that Charge #1 exerts on the dipole is

4. Electric field of a dipole + - d A E-field on the line connecting two charges when r>>d E-field on the line perpendicular to the dipole’s axis + - d A General case – combination of the above two

5. Dipole’s Potential Energy E-field does work on the dipole – changes its potential energy Work done by the field (remember your mechanics class?) Dipole aligns itself to minimize its potential energy in the external E-field. Net force is not necessarily zero in the non-uniform electric field – induced polarization and electrostatic forces on the uncharged bodies

6. Chapter 22 Gauss’s Law

7. Charge and Electric Flux Previously, we answered the question – how do we find E-field at any point in space if we know charge distribution? Now we will answer the opposite question – if we know E-field distribution in space, what can we say about charge distribution?

8. Electric flux Electric flux is associated with the flow of electric field through a surface For an enclosed charge, there is a connection between the amount of charge and electric field flux.

9. Calculating Electric Flux Amount of fluid passing through the rectangle of area A

10. Flux of a Uniform Electric Field - unit vector in the direction of normal to the surface Flux of a Non-Uniform Electric Field E – non-uniform and A- not flat

11. Few examples on calculating the electric flux Find electric flux

12. Gauss’s Law

13. Applications of the Gauss’s Law If no charge is enclosed within Gaussian surface – flux is zero! Electric flux is proportional to the algebraic number of lines leaving the surface, outgoing lines have positive sign, incoming - negative Remember – electric field lines must start and must end on charges!

14. Examples of certain field configurations Remember, Gauss’s law is equivalent to Coulomb’s law However, you can employ it for certain symmetries to solve the reverse problem – find charge configuration from known E-field distribution. Field within the conductor – zero (free charges screen the external field) Any excess charge resides on the surface

15. Field of a charged conducting sphere

16. Field of a thin, uniformly charged conducting wire Field outside the wire can only point radially outward, and, therefore, may only depend on the distance from the wire - linear density of charge

17. Field of the uniformly charged sphere Uniform charge within a sphere of radius r Q - total charge - volume density of charge Field of the infinitely large conducting plate  - uniform surface charge density

18. Charges on Conductors Field within conductor E=0

19. Experimental Testing of the Gauss’s Law