2. R 2R2R a a

3. Today… More on Electric Field: –Continuous Charge Distributions Electric Flux: –Definition –How to think about flux

4. Reminder: Lecture 2, ACT 3 Consider a circular ring with total charge + Q. The charge is spread uniformly around the ring, as shown, so there is λ = Q/2  R charge per unit length. The electric field at the origin is R x y + + + + + + + + + + + + + + + + + + + + + + (a) zero (b) (c) But how would we calculate this??

5. Electric Fields from Continuous Charge Distributions Principles (Coulomb’s Law + Law of Superposition) remain the same. Only change: Examples: line of charge charged plates electron cloud in atoms, … ++++++++++++++++++++++++++ r E(r) = ?

6. A B 2) A finite line of positive charge is arranged as shown. What is the direction of the Electric field at point A? a) up b) down c) left d) right e) up and left f) up and right 3) What is the direction of the Electric field at point B? a) up b) down c) left d) right e) up and left f) up and right L Preflight 3:

7. Charge Densities How do we represent the charge “ Q ” on an extended object? total charge Q small pieces of charge dq Line of charge :  = charge per unit length dq = dx Surface of charge:   = charge per unit area dq =  dA Volume of Charge :   = charge per unit volume dq =  dV

8. How We Calculate (Uniform) Charge Densities: Take total charge, divide by “size” Examples: 10 coulombs distributed over a 2-meter rod. 14 pC (pico = 10 -12 ) distributed over a shell of radius 1 μm. 14 pC distributed over a sphere of radius 1 mm.

9. Electric field from an infinite line charge Approach: “Add up the electric field contribution from each bit of charge, using superposition of the results to get the final field.” In practice: Use Coulomb’s Law to find the E -field per segment of charge Plan to integrate along the line… –x : from  to  OR  : from  to  ++++++++++++++++++++++++++ r E(r) = ? Any symmetries ? This may help for easy cancellations ++++++++++++++++++++++++ + ++++  x

10. Infinite Line of Charge We need to add up the E -field contributions from all segments dx along the line. Charge density = ++++++++++++++++ x y dx r' r  dE

11. Infinite Line of Charge To find the total field E, we must integrate over all charges along the line. If we integrate over , we must write r ’ and dq in terms of  and d . The electric field due to dq is: Solution: After the appropriate change of variables, we integrate and find: *the calculation is shown in the appendix ++++++++++++++++ x y dx r' r  dE

12. Infinite Line of Charge Conclusion: The Electric Field produced by an infinite line of charge is: - everywhere perpendicular to the line - is proportional to the charge density - decreases as - next lecture: Gauss’ Law makes this trivial!! ++++++++++++++++ x y dx r' r  dE

13. Summary Electric Field Lines Electric Field Patterns Dipole ~ 1/ R 3 Point Charge ~ 1/ R 2 ~ 1/ R Infinite Line of Charge Coming up: Electric field Flux and Gauss’ Law

14. The Story Thus Far Two types of electric charge: opposite charges attract, like charges repel Coulomb’s Law: Electric Fields Charges respond to electric fields: Charges produce electric fields:

15. The Story Thus Far We want to be able to calculate the electric fields from various charge arrangements. Two ways: 2.Gauss’ Law: The net electric flux through any closed surface is proportional to the charge enclosed by that surface. In cases of symmetry, this will be MUCH EASIER than the brute force method. 1.Brute Force: Add up / integrate contribution from each charge. Often this is pretty difficult. Ack! Ex: electron cloud around nucleus

16. Lecture 3, ACT 1 Examine the electric field lines produced by the charges in this figure. Which statement is true? (a) q 1 and q 2 have the same sign (b) q 1 and q 2 have the opposite signs and q 1 > q 2 (c) q 1 and q 2 have the opposite signs and q 1 < q 2 q1q1 q2q2

17. Lecture 3, ACT 1 Field lines start from q 2 and terminate on q 1. This means q 2 is positive; q 1 is negative; so, … not (a) Now, which one is bigger ? Notice along a line of symmetry between the two, that the E -field still has a positive y component. If they were equal, it would be zero; This indicates that q 2 is greater than q 1 Examine the electric field lines produced by the charges in this figure. Which statement is true? (a) q 1 and q 2 have the same sign (b) q 1 and q 2 have the opposite signs and q 1 > q 2 (c) q 1 and q 2 have the opposite signs and q 1 < q 2 q1q1 q2q2

18. Electric Dipole: Lines of Force Consider imaginary spheres centered on : a a) + q (blue) b b) -q (red) c c) midpoint (yellow) All lines leave a) All lines enter b) Equal amounts of leaving and entering lines for c)

19. Electric Flux Flux: Let’s quantify previous discussion about field- line “counting” Define: electric flux   through the closed surface S “ S ” is surface of the box

20. Flux How much of something is passing through some surface Ex: How many hairs passing through your scalp. Two ways to define 1.Number per unit area (e.g., 10 hairs/mm 2 ) This is NOT what we use here. 2.Number passing through an area of interest e.g., 48,788 hairs passing through my scalp. This is what we are using here.

21. Electric Flux What does this new quantity mean? The integral is over a CLOSED SURFACE Since is a SCALAR product, the electric flux is a SCALAR quantity The integration vector is normal to the surface and points OUT of the surface. is interpreted as the component of E which is NORMAL to the SURFACE Therefore, the electric flux through a closed surface is the sum of the normal components of the electric field all over the surface. The sign matters!! Pay attention to the direction of the normal component as it penetrates the surface… is it “out of” or “into” the surface? “Out of” is “+” “into” is “-”

22. How to think about flux We will be interested in net flux in or out of a closed surface like this box This is the sum of the flux through each side of the box –consider each side separately Let E -field point in y -direction –then and are parallel and Look at this from on top –down the z -axis surface area vector: w “ S ” is surface of the box x y z

23. How to think about flux Consider flux through two surfaces that “intercept different numbers of field lines” –first surface is side of box from previous slide –Second surface rotated by an angle  case 1 case 2  case 1 case 2 E -field surface area E S Case 2 is smaller! Flux:

24. The Sign Problem For an open surface we can choose the direction of S -vector two different ways –to the left or to the right –what we call flux would be different these two ways –different by a minus sign right left A differential surface element, with its vector For a closed surface we can choose the direction of S -vector two different ways –pointing “in” or “out” –define “out” to be correct –Integral of E dS over a closed surface gives net flux “out,” but can be + or -

25. E 1 2 Wire loops (1) and (2) have the same length and width, but differences in depth. Wire loops (1) and (2) are placed in a uniform electric field as shown. Compare the flux through the two surfaces. a) Ф 1 > Ф 2 b) Ф 1 = Ф 2 c) Ф 1 < Ф 2 5) Preflight 3:

26. 6) A cube is placed in a uniform electric field. Find the flux through the bottom surface of the cube. a) Ф bottom < 0 b) Ф bottom = 0 c) Ф bottom > 0 Preflight 3:

27. Lecture 3, ACT 2 2A Imagine a cube of side a positioned in a region of constant electric field as shown Which of the following statements about the net electric flux  E through the surface of this cube is true? (a)  E =  (b)  E  2 a  (c)  E  6 a  a a 2B R 2R2R Consider 2 spheres (of radius R and 2 R ) drawn around a single charge as shown. –Which of the following statements about the net electric flux through the 2 surfaces (  2 R and  R ) is true? (a)  R <  2 R (b)  R =  2 R (c)  R >  2 R

28. Lecture 3, ACT 2 2A Imagine a cube of side a positioned in a region of constant electric field as shown Which of the following statements about the net electric flux  E through the surface of this cube is true? (a)  E =  (b)  E  2 a  (c)  E  6 a  a a The electric flux through the surface is defined by: on the bottom face is negative. ( dS is out; E is in) on the top face is positive. ( dS is out; E is out) Therefore, the total flux through the cube is: is ZERO on the four sides that are parallel to the electric field.

29. 2B R 2R2R Consider 2 spheres (of radius R and 2 R ) drawn around a single charge as shown. –Which of the following statements about the net electric flux through the 2 surfaces (  2 R and  R ) is true? (a)  R <  2 R (b)  R =  2 R (c)  R >  2 R Lecture 3, ACT 2 Look at the lines going out through each circle -- each circle has the same number of lines. The electric field is different at the two surfaces, because E is proportional to 1 / r 2, but the surface areas are also different. The surface area of a sphere is proportional to r 2. Since flux =, the r 2 and 1/ r 2 terms will cancel, and the two circles have the same flux! There is an easier way. Gauss’ Law states the net flux is proportional to the NET enclosed charge. The NET charge is the SAME in both cases. But, what is Gauss’ Law ???--You’ll find out next lecture!

30. Summary Electric Fields of continuous charge distributions Electric Flux: –How to think about flux: number of field lines intercepting a surface, perpendicular to that surface ++++++++++++++++++++++++++ r E ( r ) = Next Time: Gauss’ Law

31. Appendix Infinite Line of Charge We use Coulomb’s Law to find dE : What is r’ in terms of r ? What is dq in terms of dx ? Therefore, ++++++++++++++++ x y dx r' r  dE

32. x and  are not independent! x = r tan  dx = r sec 2  d  ++++++++++++++++ x y dx r' r  dE We are dealing with too many variables. We must write the integral in terms of only one variable  or x )  We will use . We still have x and  variables. Infinite Line of Charge

33. Components: Integrate: ExEx ++++++++++++++++ x y dx r' r  dE  EyEy

34. Infinite Line of Charge Now The final result: ExEx ++++++++++++++++ x y dx r' r  dE  EyEy