1. Interaction of Charged Objects Attraction: can happen also for like-charged objects! Repulsion: can happen only for like-charged objects! Intervening matter does not “block” the E field The resulting field is a superposition of two fields: Field of the charge plus the field of induced dipoles. + - +

2. Clicker Question A B D C What is the direction of the electric field at X due to the dipole?

3. Clicker Question A B D C What is the direction of the electric field at X due to the plastic block?

4. Clicker Question A B D C What is the direction of the NET electric field at X?

5. Clicker Question The force of one of the permanent dipoles on the other is: A) Attractive B) Repulsive C) The force is zero

6. Different materials respond differently to electric field Conductor: contains mobile charges that can move through material Insulator: contains no mobile charges Conductors and Insulators

7. Insulator: Electrons are bound to the atoms or molecules. Electrons can shift slightly (<1 Å), but remain bound to the molecule. Individual atoms or molecules can be polarized by external electric field. There are a lot of molecules – the net effect produced by the induced dipoles can be very large. Polarization of Insulators

8. Diagram showing polarization of an insulator: Dipoles: exaggerated in size; stretch: degree of polarization No mobile charges: excess charges stay where they are Polarization of Insulators

9. Field E at a location of a molecule is a superposition of the external applied field and the field created by other induced dipoles: Simplifying assumption: Low Density Approximation

10. There are charges which can move freely throughout the material E In contrast to an insulator, where electrons and nuclei can move only very small distances, the charged particles in a conductor are free to move large distances. Polarization of conductors differs from that of insulators. Conductors

11. Salt water: Na + and Cl - H + and OH - Apply external electric field Ionic Solutions are Conductors When an electric field is applied to a conductor, the mobile charged particles begin to move in the direction of the force exerted on them by the field. As the charges move, they begin to pile up in one location, creating a concentration of charge  creates electric field. The net electric field is the superposition of the applied field and field created by the relocated charges.

12. Assumption: charges will move until E net =0 (static equilibrium) It is not a shielding effect, but a consequence of superposition! Proof: by contradiction: Mobile ions will move This is not equilibrium Assume E net ≠0 Assumption E net ≠0 is wrong E net =0 Ionic Solutions are Conductors

13. Your body consists mainly of salt water Polarization of salt water has much higher effect than polarization of atoms! Polarization of Salt Water in the Body

14. Positive atomic cores and mobile-electron sea Electrons are not completely free – they are bound to the metal as a whole. Metal lattice There is no net interaction between mobile electrons A Model of a Metal We will return to this idea when we discuss the force on a current carrying wire in a magnetic field.

15. Simplified diagram of polarized metal Note: It is not charged! Net charge is still zero Metal in Electric Field

16. In static equilibrium: E net = 0 everywhere inside the metal! Mobile charges on surface rearrange to achieve E net = 0 Actual arrangement might be very complex! It is a consequence of 1/r 2 distance dependence E net = 0 only in static equilibrium! Electric Field inside Metal

17. - No net interaction between mobile electrons Forget previous velocity after collision conductivity (  )  μ Drude Model of Electron Motion in a Metal

18. Excess charges in any conductor are always found on an inner or outer surface! Excess Charge on Conductors

19. ConductorInsulator Mobile chargesyesno Polarization entire sea of mobile charges moves individual atoms/molecules polarize Static equilibrium E net = 0 insideE net nonzero inside Excess chargesonly on surface anywhere on or inside material Distribution of excess charges Spread over entire surfacelocated in patches Conductors versus Insulators

20. Discharging by contact: On approach: body polarizes On contact: charge redistributes over larger surface Grounding: connection to earth (ground) – very large object Charging and Discharging

21. Charging by Induction

23. An object can be both charged and polarized On a negatively charged metal ball excess charge is spread uniformly all over the surface. What happens if a positive charge is brought near? + Exercise

24. Splitting universe into two parts does not always work. +q If q is so small that it does not appreciably alter the charge distribution on the sphere, then we can still use the original field: Otherwise, we must calculate new field: When the Field Concept is less Useful