Problem Assignment #1: Electrostatics and Dirac Delta Functions, Assignments of Physics

Problem assignments for a university-level electrostatics course, focusing on the use of dirac delta functions to represent various charge distributions and their corresponding potentials. The assignments include calculations for charge distributions in spherical and cylindrical coordinates, as well as proving the limit of a specific function approaches a dirac delta function.

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Pre 2010

Uploaded on 08/30/2009

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Problem Assignment #1
A. W. Stetz
October 4, 2007
These problems are due Friday, Oct. 12.
1. Using the Dirac delta functions in the appropriate coordinates, express
the following charge distributions as three-dimensional charge densities
ρ(x).
(a) In spherical coordinates, a charge Quniformly distributed over a
spherical shell of radius R.
(b) In cylindrical coordinates, a charge λper unit length uniformly
distributed over a cylindrical surface of radius b.
(c) In cylindrical coordinates, a charge Qspread uniformly over a
flat circular disc of negligible thickness and radius R.
(d) The same as part (c), but using spherical coordinates.
2. The time-averaged potential of a neutral hydrogen atom is given by
φ=qeαr
r1 + αr
2
where qis the magnitude of the electronic charge, and α1=a0/2, a0
being the Bohr radius. Find the distribution of charge (both continu-
ous and discrete) that will give this potential and interpret your result
physically.
3. Given the definition,
D(x, α) = 1
2πα2ex2/2α2,
prove that in the limit α0
D(x, α) = δ(x).
1

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Problem Assignment

A. W. Stetz

October 4, 2007

These problems are due Friday, Oct. 12.

  1. Using the Dirac delta functions in the appropriate coordinates, express the following charge distributions as three-dimensional charge densities ρ(x).

(a) In spherical coordinates, a charge Q uniformly distributed over a spherical shell of radius R. (b) In cylindrical coordinates, a charge λ per unit length uniformly distributed over a cylindrical surface of radius b. (c) In cylindrical coordinates, a charge Q spread uniformly over a flat circular disc of negligible thickness and radius R. (d) The same as part (c), but using spherical coordinates.

  1. The time-averaged potential of a neutral hydrogen atom is given by

φ = q

e−αr r

αr 2

where q is the magnitude of the electronic charge, and α−^1 = a 0 /2, a 0 being the Bohr radius. Find the distribution of charge (both continu- ous and discrete) that will give this potential and interpret your result physically.

  1. Given the definition,

D(x, α) =

2 πα^2

e−x

(^2) / 2 α 2 ,

prove that in the limit α → 0

D(x, α) = δ(x).