Resources on non-spherical conductor surface charges

AI Thread Summary
Charges on non-spherical conductors tend to concentrate at sharp edges, a phenomenon that requires a rigorous mathematical treatment involving Poisson's equation. Analytical solutions are typically limited to highly symmetric cases, while more complex geometries necessitate numerical methods like finite-element analysis. The discussion highlights the need for resources that provide analytical methods or approximations for understanding charge distribution on pointed surfaces. A textbook example illustrates charge distribution between two connected conducting spheres, emphasizing the relationship between potential and charge. Overall, the conversation seeks guidance on rigorous mathematical approaches to this electrostatic behavior.
albertrichardf
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Hi all,
I know qualitatively that charges tend to concentrate on sharp edges of conducting surfaces. I have tried searching online for a mathematical treatment of such a phenomenon, but I cannot find anything that's quite rigorous. I'd appreciate it if someone could guide me towards such resources.
Thank you.
 
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Albertrichardf said:
Hi all,
I know qualitatively that charges tend to concentrate on sharp edges of conducting surfaces. I have tried searching online for a mathematical treatment of such a phenomenon, but I cannot find anything that's quite rigorous. I'd appreciate it if someone could guide me towards such resources.
Thank you.

Define "mathematical treatment".

If you want a plug-and-chug equation, there is no such thing. This is really a complex boundary-value problem involving finding the solution to Poisson's equation. Only the simplest and highly-symmetric cases will you find an analytical solution. Otherwise, you have to solve it numerically, typically using finite-element analysis.

Zz.
 
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Likes BvU and vanhees71
Thanks for answering. I mean, are there any analytical methods to solve, or approximate a solution to Poisson's equation in these cases? Or at least show mathematically, that the charges tend to concentrate at the tip of a pointed surface?
 
The textbook proof goes this way.
Consider two conducting spheres, with radii ##R_1## and ##R_2##, separated by a large distance ##r \gg R_1,R_2## but connected by a wire. The surfaces have the same electric potential.
If the total charge is ##Q_1+Q_2##, what are ##Q_1## and ##Q_2## (how must that total charge be distributed)?
See, e.g., https://www.feynmanlectures.caltech.edu/II_06.html#Ch6-S11
 
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