Thin disc above grounded plane

[ducks]

Homework Statement

A thin disk of radius R consists of a uniformly distributed total charge Q. The disk lies a distance D above a grounded perfectly conducting plane. The disk and the plane are parallel. Set the conducting plane in the x-y axis, and the z axis through the center of the disk.
R=0.1 m, the distance D = 2R = 0.2 m, and the charge Q=1/(9E9) Coulomb

Compute the potential along the axis through the center of the charged disk

Homework Equations

If it was a single point charge:
V(x,y,z) = 1/4*∏*\epsilon * [ q/ \sqrt{x^2+y^2+(z-d)^2} - q/ \sqrt{x^2+y^2+(z+d)^2} ]

The Attempt at a Solution

I have a feeling I would solve this using the method of images with an imaginary disc of -q charge below the conducting plane. Would this be the same for the thin disc? With the given value turning it into this?

[ 1/ \sqrt{x^2+y^2+(z-d)^2} - 1/ \sqrt{x^2+y^2+(z+d)^2} ]

My second problem is to to calculate numerically the potential everywhere in space above the conducting plane. Could I get any hints as to how to do this?

 

[diazona]

I have a feeling I would solve this using the method of images with an imaginary disc of -q charge below the conducting plane.

That does seem like the way to go. Just keep in mind that the charge is a disc, not a point, so you can't just use the point charge formula unaltered. You'll have to do an integral.

 

[rude man]

I would run a Gaussian surface, a right circular cylinder, with one flat surface located within the disk (and parallel to it) to a plane a distance r between the disk and the ground plane, compute E(r), integrate E(r) from the disk to the ground plane, with the constant of integration such that V(D-r) = 0.

You can also do it by the image method, you'd get the same result. Since you would not extend the Gaussian variable surface beyond r = D there would be no difference in the equations.

 

[ducks]

I figured out the z axis part since it forms a right triangle. I can't wrap my head around how I would measure the potential at a point not on the z axis.

 

[rude man]

I didn't see that part of the problem. That's a lot more difficult all right.

I would go with V(r) = k∫σ*dA/r integrated over disk surface A
r = distance from element of charge σ*dA
k = 9e9 SI
σ = surface charge density = constant thruout disk = Q/πR^2
A = disk area

But you've probably figured that far already.
r = distance from point (x0, y0) on disk defined by surface (x^2 + y^2 = R^2, D)
to arbitrary poit (x,y,z).

Just a math problem ... :-)