1. Electrostatics
Coulomb’s Law

2. Coulomb’s Law F = (kq1q2)/r2 K = 9 x 109 Nm2/C2
Positive force means repulsion
Negative force means attraction

3. Example problem
4 m
A charge q1 = 4 μC is positioned at the origin. A charge of q2 = 9 μC is positioned at x = 4 m. Where on the x-axis can a charge q3 be placed so that the force is zero? q1 q3 q2

4. Solution (kq1q3)/x2 = (kq2q3)/ (4-x)2 kq1(4-x)2 = kq2 x2
4 μC (4-x)2 = 9 x2
4(16-8x+x2) = 9x2
5x2 +32x – 64 = 0
x = 1.6 m

5. Example problem
Table salt is a crystal with a simple cubic structure with Na+ and Cl- ions alternating on adjacent lattice sites. The distance between ions is a = 2.82 x m. a)What force does Na+ experience due to one of its Cl- neighbors? B)What force does a Cl- ion experience due to a neighboring Na+? c)What force does an Na+ ion at the origin experience due to Cl- ions at (a,0,0) and (0,a,0)?

6. Solution
A) F = kq1q2/r2 = [9 x 109 (1.6 x10-19 C)2]/(.282 x m)2 = 2.9 x 10-9 N
B) same as a by Newton’s Third Law
C) F = F1 + F2 = 2.9 x 10-9 (i + j) N = √(2.9 x 10-9)2 + (2.9 x 10-9 )2 = 4.1 x 10-9 N

7. Electric Field Vector Quantity
At every point in space it has a magnitude and direction
The total electric field at any point is the sum of the electric fields due to all charges that are present
Unit: N/C
Always point away from positive charge and toward negative charge

8. Problem
Find the force on a Ca+2 ion placed in an electric field of 800 N/C directed along the positive z-axis.
Solution:
F = qE
q = 2e
F = 2e(800N/C)
2.56 x N

9. Electric Field
E = F/q
F = kqQ/r2
E = kqQ/qr2
E = kQ/r2

10. Problem 2
A point charge q = -8.0nC is located at the origin. Find the electric field vector at the field point x = 1.2 m and y = -1.6 m.

11. Solution
E = - 11 N/C i and 14 N/C j

12. Problem 3
Four identical charges are placed on the corners of a square of side L. Determine the magnitude and direction of the electric field due to them at the midpoint of one of the square’s sides.

13. Solution…
For B and D the electric fields are the same and opposite so thy cancel each other out. B EC A P EA C D
E = 2kq/(cos2θL2)

14. Problem 4
An electric dipole consists of +q and –q and separated by a distance of 2a. If the charges are positioned at (0,0,a and (0,0,-a) determine the electric field at a point a distance of z from the origin on the z-axis, where z >> 2a.

15. Charge Distributions and E-fields
ΔE = k ΔQ/r2 r
E = k Σi Δqi/ri2 r
E = k lim Σ Δqi/ri2 r = k ∫dq/r2 r

16. Linear charge distribution
Charge Q is distributed on a line of length l, the linear charge density
λ = Q/l
dq = λ dl

17. Surface Area Charge Distribution
Charge Q is distributed on a surface area A, the surface density
δ = Q/A
dq = δ dl

18. Volume Charge Distribution
Charge Q is distributed uniformly throughout a volume V, the volume charge density
ρ = Q/V
dq = ρ dl

19. Problem 1
A rod of length l has a uniform positive charge per unit length, λ, and a total charge, Q. Calculate the electric field at a point P along the axis of the rod and a distance a from one end.

20. Problem 2
A ring of radius a carries a uniformly distributed positive charge Q. Calculate the E field due to the ring at a point P lying a distance x from its center along the central axis perpendicular to the plane of the ring.