How to Find Potential Difference on a Conical Surface with Uniform Charge?

  • Thread starter Thread starter bigplanet401
  • Start date Start date
  • Tags Tags
    Potential
Click For Summary
SUMMARY

The discussion focuses on calculating the potential difference between the vertex and the center of the top of a conical surface with a uniform surface charge density, denoted as \(\sigma\). The initial approach involved integrating over the conical surface using the formula \(V(\mathbf{r}) = \frac{1}{4\pi\epsilon_0} \int d\mathbf{a} \frac{\sigma(\mathbf{r}^\prime)}{|\mathbf{r} - \mathbf{r}^\prime|}\), which was deemed incorrect. A second method using charge density \(\lambda\) and potential from rings was suggested, emphasizing the need for proper integration setup to account for the geometry of the cone.

PREREQUISITES
  • Understanding of electrostatics and electric potential
  • Familiarity with calculus, particularly integration techniques
  • Knowledge of surface charge density concepts
  • Experience with cylindrical and conical coordinate systems
NEXT STEPS
  • Study the integration of electric potential for non-uniform charge distributions
  • Learn about the method of rings in electrostatics
  • Explore the derivation of potential due to surface charge distributions
  • Investigate the application of cylindrical coordinates in electrostatics problems
USEFUL FOR

Students and professionals in physics, particularly those studying electrostatics, as well as educators seeking to understand complex charge distribution problems.

bigplanet401
Messages
101
Reaction score
0
Hi,

A conical surface (an empty ice-cream cone) carries a uniform surface charge \sigma. The height of the cone is h, and the radius of the top is R. Find the potential difference between points a (the vertex) and b (the center of the top.)

I've tried integrating over the conical surface (zenith \phi fixed):

<br /> V(\mathbf{r}) = \frac{1}{4\pi\epsilon_0} \int d\mathbf{a} \frac{\sigma(\mathbf{r}^\prime)}{|\mathbf{r} - \mathbf{r}^\prime|} \quad \rightarrow \quad <br /> \frac{1}{4\pi\epsilon_0} \int r^{\prime 2} dr^\prime \, d\theta^\prime<br /> \frac{\sigma}{\sqrt{1 - r^{\prime 2} \cos^2 \phi}} \, ,<br />

but I think that's wrong. Next I tried building up from a series of rings with charge density \lambda:

<br /> V_{\text{ring}} = \frac{\lambda}{2 \epsilon_0} \frac{R}{\sqrt{R^2 + z^2}} \, ;<br />

unfortunately, I don't know how to set up the integration for this. Any help is appreciated,hopefully sooner than later--my written qualifier is ~3 weeks away!
 
Physics news on Phys.org
There shouldn't be any angular dependence in the integrand if you choose to use the first method, so the integral as you have it set up now is wrong. For each area element rdrd\phi in the xy plane, think about the corresponding portion of the surface of the cone. Find the amount of charge in this surface element (this will involve the slope of the cone), and the distance from it to the point you want to calculate the potential. Then integrate over the disk in the xy plane corresponding to the cone.

If you want to use the second method, you'll need to think of rings on the cone corresponding to some dr or dz and then integrate over the height or radius of the cone. For example, if you choose to use dz, find the charge between z and z+dz as a function of z, then find the potential due to this ring, which will be proportional to dz, and then integrate over z.
 
Last edited:

Similar threads

Replies
6
Views
3K
Replies
11
Views
2K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 17 ·
Replies
17
Views
2K
  • · Replies 23 ·
Replies
23
Views
2K
Replies
64
Views
6K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 18 ·
Replies
18
Views
1K