**Problem 1** [5 points]
Consider a point charge q a distance d in front of a plane conducting slab of thickness w, as shown below. The slab has a fixed net charge Q on it. Find the electric field on both sides of the slab. Find the force between the charge q and the slab. For this problem, assume that the side area of the slab A is finite, so that the average surface charge Q/2A is finite; however you make work the problem out ignoring edge effects, i.e. assuming the plane is effectively infinite.

**Problem 2** [10 points]
A line charge λ is placed parallel to, and a distance R away from, the axis of a conducting cylinder of radius b that is held at fixed voltage such that the potential vanishes at infinity. Find

a) the magnitude and position of the image charge(s)

b) the potential at any point (expressed in polar coordinates with the origin at the axis of the cylinder and the direction from the origin to the line charge as the x axis)

c) the induced surface charge density, and plot it as a function of angle for R/b = 2 and 4 in units of λ/2πb

d) the force on the line charge per unit length

**Problem 3** [10 points]
A surface charge density σ(φ) = a sin(5φ) is glued over the surface of an infinite cylinder of radius R (φ is the polar angle).

a) Find the potential for r<R inside the cylinder.

b) Find the potential for r>R outside the cylinder.

**Problem 4** [10 points]
Two concentric spherical shells of radii R_{1} and R_{2}, with R_{1}<R_{2}, are fixed with the following values of the electrostatic potential:

φ(R_{1}, θ) = φ_{1}cosθ and
φ(R_{2}, θ) = φ_{2}

where φ_{1} and φ_{2} are constants and θ is the usual azimuthal spherical angle. Find the electrostatic potential for:

a) r<R_{1}, inside the inner shell

b) r>R_{2}, outside the outer shell

c) R_{1}<r<R_{2}, between the two shells

d) Find the surface charge density σ(θ) on each of the two shells.

**Problem 5** [15 points]
a) Consider an infinitesmally thin charged disk of radius R and uniform surface charge density σ_{o}, that is lying in the xy plane centered on the orign. Using the Coulomb formula for the potential,

φ(**r**) = ∫ da´ |
σ(**r**´) |**r** - **r**´| |

do the integral to find the exact value of the potential φ for points along the z axis, both above and below the disk (make sure you get this part correct before proceeding with the following parts!). [5 pts]

b) Since the above problem of the charged disk has rotational symmetry about the z axis, we can express the solution for the potential φ(**r**) in terms of a Legendre polynomial series using the method of separation of variables. In this case, the "boundary condition" that determines the unknown coefficients of this series is the requirement that the potential agree with the known exact values along the z axis, as computed in part (a). Find the coefficients of this expansion up to order l=5, for |**r**|>R and |**r**|<R, both *above* and *below* the disk. (*Hint*: read Jackson section 3.3) [5 pts]

c) Using your results of part (b), compute the electric field **E** just above and just below the disk, and explicitly show that the discontinuity in **E** is given by the surface charge density σ_{o}, as we know from general principles that it must be. [5 pts]