Electric field of periodic charge density.

JoshThompson42
Messages
3
Reaction score
0

Homework Statement


Find electrostatic field and potential created by a two-dimensional charge density:
\rho \sin (kx) \cos (ky) \delta (z)
at the distance d from the the plane z=0 where the charge is placed (taking into account that it is embedded in a three dimensional space).
In your calculations you are required to use Fourier analysis.

Homework Equations

The Attempt at a Solution


My initial thought was to use the differential form of Gauss's law:
\nabla \cdot E = \frac{\rho}{\epsilon_0}

However I am unsure of where Fourier analysis comes into play, any pointers as to where to go from here would be great. My instinct tells me that the delta function should be what gets the Fourier treatment, however it isn't periodic.
 
Physics news on Phys.org
What is the potential for a point-charge? To extend this to 2-dimensional charge distributions, you'll need an integral. And I guess the evaluation of this integral will need Fourier analysis.
 
mfb said:
What is the potential for a point-charge? To extend this to 2-dimensional charge distributions, you'll need an integral. And I guess the evaluation of this integral will need Fourier analysis.
To make Fourier analysis more obvious, I would start from Poisson's equation for the potential: given the charge distribution, you have to guess oscillating functions for the x and y components which leads to Fourier analysis to determine the coefficients. The z-component is less obvious though, and you'd have to use the ±z symmetry of the problem... Incidentally, the full solution for arbitrary z comes rather easily using Fourier transform.
 
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top