1. COULOMB’S LAW, E FIELDS

2. Class Activities Coulomb’s Law

3. Class Activities: Charge Distibutions

4. Two charges +Q and -Q are fixed a distance r apart. The direction of the force on a test charge -q at A is… A.Up B.Down C.Left D.Right E.Some other direction, or F =0

5. Two charges +q and -q are on the y- axis, symmetric about the origin. Point A is an empty point in space on the x- axis. The direction of the E field at A is… A.Up B.Down C.Left D.Right E.Some other direction, or E = 0, or ambiguous 2.3 +q x y -q A

6. How is the vector related to r 1 and r 2 ? r2r2 r1r1 2.1b

7. Coulomb's law: In the fig, q1 and q2 are 2 m apart. Which arrow can represent ? q1q2 A BC D) More than one (or NONE) of the above E) You can't decide until you know if q1 and q2 are the same or opposite signed charges

8. What is ("from 1 to the point r") here? +q r 1 =(x 1,y 1 ) -q r=(x,y) 2.2

9. Can I always use Coulomb’s Law to calculate the force on a small charge at any point in vacuum if I know the location of all charges for all times? (Assume no conductors or dielectrics are present.) A)Yes, of course! (It’s not just a good idea, it’s the law) B)No. Coulomb’s law works only for specific situations. C)I don’t know and my neighbor has no clue either. Clicker code is AB

10. Only click when you are DONE with page 1 (Part 1 i-iii) Is the answer to part 1- iii A)A sum? B)An integral over dy? C)An integral over something else?

11. Tutorial 1, part 2- Script r Only after you finish Part 2, what is in part 2-iv ? E) None of these!

12. Only when you finish Part 3-vi: What is here? A) B)a C) D) z E) Something completely different!! P=(0,0,z) a x y dl' 2.13

13. 5 charges, q, are arranged in a regular pentagon, as shown. What is the E field at the center? A) Zero B) Non-zero C) Really need trig and a calculator to decide q q q q q 2.5

14. 1 of the 5 charges has been removed, as shown. What’s the E field at the center? q q q q A) +(kq/a 2 ) j B) -(kq/a 2 ) j C) 0 D) Something entirely different! E) This is a nasty problem which I need more time to solve +x +y a 2.6

15. To find the E- field at P=(x,y,z) from a thin line (uniform linear charge density ): What is ? A) XB) y' C) D) E) Something completely different!! P=(x,0,0) x y dl' r' r 2.10

16. P=(x,0,0) x y dl' r'= (0,y',0) r 2.11

17. ,so P=(x,0,0) x y dl' r'= (0,y',0) r 2.11

18. To find the E- field at P from a thin ring (radius R, uniform linear charge density ): what is ? P=(0,0,z) R x y dl' B E) NONE of the arrows shown correctly represents A C D 2.12

19. To find the E- field at P from a thin ring (radius a, uniform linear charge density ): what is ? A) B) a C) D) z E) Something completely different!! P=(0,0,z) a x y dl' 2.13

20. Griffiths p. 63 finds E a distance z from a line segment with charge density : What is the approx. form for E, if z>>L? A) 0 B) 1 C) 1/zD) 1/z^2 E) None of these is remotely correct. x (0,0,z) -L +L 2.16

21. Griffiths p. 63 finds E a distance z from a line segment with charge density : What is the approx. form for E, if z<<L? A) 0 B) 1 C) 1/zD) 1/z^2 E) None of these is remotely correct. x (0,0,z) -L +L 2.16

22. D) None of these To find E at P from a negatively charged sphere (radius R, uniform volume charge density  ) using what is (given the small volume element shown)? P=(x,y,z) x y z (x’,y’,z’) R A B C 2.14

23. A) B) C) D) E) None of these P=(X,Y,Z) x y z (x,y,z) R 2.15 dq

24. A) B) C) D) E) None of these P=(X,Y,Z) x y z (x,y,z) R 2.15