START for EXAM #1

Assignment #1 Section 22-3 Date Due: Fri. Sept. 26
Assignment #2 Section 22-4 Date Due: Mon. Sept. 29
Assignment #3 Section 23-1 Date Due: Tue. Sept. 30
Assignment #4 Section 23-2 Date Due: Wed. Oct. 1
Assignment #5 Section 24-2 Date Due: Fri. Oct. 3
Assignment #6 Section 24-4 & 24-3 Date Due: Mon. Oct. 6
EXAM #1: Wednesday Oct. 8 - Chapters 22, 23, & 24

Topics for Exam #1

If you want to match the answers in brackets to all 3 significant figures then you will have to use the value of Coulomb's constant and the electric charge to be k = 9.00x109 N m2/C2 and e =1.60x10-19C


Assignment #1 Section 22-3 Date Due: Fri. Sept. 26 Coulomb's Law

1. Two charges q1 = -7.35 mC and q2 = -2.90 mC {q1 = -3.45 mC and q2 = +4.80 mC} are placed 76.0 cm apart. If q1 is to the left of q2,


Assignment #2 Section 22-4 Date Due: Mon. Sept. 29 Electric Field of Point Charges

2. Two charges (q1 = -3.40 mC and q2 = +5.10 mC) {( q1 = +2.60 mC and q2 = -1.75 mC)} are placed in such a way that charge q1 is 384 cm above the origin on the y-axis and charge q2 is placed 739 cm to the right of the origin along the x-axis.


Assignment #3 Section 23-1 Date Due:Tue. Sept. 30 Charge Distribution

3-1. A charge of 44.0 mC is placed on a horizontal rod that is 11.5 cm {2.70 m} long in such a way that the charge is divided equally into two + 22.0 mC charges and placed on the ends of the rod. ( I suggest you place the origin at the left end of the rod and not at the rods center.)

3-2. A charge of 44.0 mC is placed on a horizontal rod that is 11.5 cm {2.70 m} long in such a way that the charge is distributed evenly along the rod.

Note that Tipler does the { } example in section 23-1. What is not clear in his example that r in Column’s law always has to be positive. In particular, r = xo – x since xo > x in the {} example but this is not true the nonbracketed problem. If you use r = xo - x you will get the correct numerical answer but this not correct and it will not work in 3-3.

3-3. A charge of 44.0 mC is placed on a rod that is 11.5 cm {2.70 m} long in such a way that the charge density along the rod increases uniformly from left to right. As a result the linear charge density is given by l = a x when the left end of the rod is at the origin; here a is a constant.


Assignment #4 Section 23-2 Date Due: Wed. Oct. 1 Gauss's Law

4-1. A non-conducting sphere of radius 1.50 m has a total charge Q distributed through out the interior of the sphere in such a way that the charge density falls off as r(r) = a/ r where a = 25.5 mC/m 2 {r(r) = b/ r2 where b = 33.0 mC/m}. (See example 23-7 in Tipler}

4-2. A charge of + 120 mC is transferred to the outside of a spherical conducting shell with an inner radius 16.0 cm and an outer radius of 22.0 cm. Next a -48.0 mC {+390 mC} point charge is placed at the center of the conducting shell.


Assignment #5 Section 24-2 Date Due: Fri. Oct. 3 Potential of Point Charges

5-1. Two point charges q1 = 13.5 nC & q2 = -18.0 nC { q1 = -88.0 nC & q2 = 360 nC} are located at the fixed positions of x1 = 22.0 cm and x2 = 96.0 cm on the x-axis.


Assignment #6 Section 24-4 & 24-3 Date Due: Mon. Oct. 6 Potential of Line Charge

6-1. A charge of 44.0 mC is placed on a rod that is 11.5 cm {2.70 m} long in such a way that the charge is spread uniformly along the rod. This is thew same setup as homework problem 3-2.


EXAM #1 Wednesday

October 8 - CHAPTERS 22, 23, & 24

Electric Charge & Coulomb's Law

Charge Distributions

Electric Field

Gauss's Law & Electric Flux

Electric Potential