Method of Images two parallel pipes at potentials of 0 & +V

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Discussion Overview

The discussion revolves around the method of images applied to two parallel conducting pipes at different potentials, specifically comparing scenarios with potentials of -V and +V versus 0 and +V. Participants explore the implications of these configurations on potential distributions and the feasibility of using the method of images and superposition to solve the problem.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes a scenario with two parallel pipes at potentials -V and +V and questions the applicability of the method of images when the potentials are changed to 0 and +V.
  • Another participant suggests using superposition to find the potential distribution by combining the solutions for each pipe treated individually.
  • A request for clarification indicates that some participants find the explanation of superposition and charge density challenging to understand.
  • Further elaboration is provided on determining charge densities and potentials for the pipes based on their configurations.
  • One participant expresses confusion about achieving a potential of 0 on one pipe while simultaneously achieving a potential of +2V on the other, questioning the feasibility of such a combination of charges.
  • Another participant proposes that one pipe will have a small negative charge while the other has a larger positive charge, suggesting a superposition of oppositely charged pipes and the same charge configuration.
  • Concerns are raised about the distortion of equipotential surfaces when both pipes carry the same charge, contrasting this with the case of oppositely charged pipes.
  • A participant inquires about solutions for two conducting pipes both at a potential of +V.

Areas of Agreement / Disagreement

Participants express varying degrees of understanding and interpretation of the method of images and superposition. There is no consensus on the best approach to achieve the desired potentials, and multiple competing views remain regarding the configurations and their implications.

Contextual Notes

Participants note limitations in understanding the implications of charge distributions and potential calculations, as well as the challenges in applying superposition effectively in different scenarios.

Erwin Derek
Consider the scenario where there are two parallel conducting pipes of radius R separated by a distance d, with pipe 1 at a potential of -V and pipe 2 at a potential +V. I have seen from many sources that there is a very easy method of images solution to the potential outside the pipes, given that the potential goes to 0 at \infty.

 

Now I thought of an alternate scenario where the only difference is that instead of -V and +V it is now 0 and +V. Can this still be solved with method of images?

I have tried using two line charges of unequal charge and the equipotential surfaces end up being slightly distorted circles, so that doesn't work.

Otherwise, how can we do this with separation of variables?
 
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Superposition still applies. You can use the original solution to find the potential distribution if only one pipe is charged, you can find suitable charges for the two pipes and then add two of these solutions together.
 
Could you please elaborate more, I'm not sure I completely understood that?

Everything after the first sentence flew over my head :P
 
There were just twos sentences! ;)

Find the original symmetric solution, determine the charge density on both pipes. Take one of them, determine the field it produces and find the corresponding potentials of the pipes. Then find a combination of (charge on pipe 1) and (charge on pipe 2) to get the potentials at the pipes right.
 
I feel like I understand what you're saying but I'm having trouble following this for some reason--

Let's say in the original scenario we have two pipes -V and +V, so now we found some charges L_1=-\lambda and L_2=+\lambda, so suppose each of these produces a potential on pipes 1 and 2 as V_{11}, V_{12}, V_{21}, and V_{22}, so now V_{11}+V_{21}=-V for all points on pipe 1 and V_{12}+V_{22}=+V for all points on pipe 2.

Now I want a scenario with, let's say two pipes 0 and +2V. I need to find a combination of L_1 and L_2 that will produce these potentials on the surface of the pipes?

Just considering the 0 pipe alone, how would this be possible? Any combination of the pipes that would produce a 0 potential on this pipe will also zero out the potential on the other pipe, and if I clone some more charges to try getting pipe 2's to +2V, won't I break the 0 potential on pipe 1?
 
Pipe 1 will have a small negative charge, pipe 2 will have a larger positive charge.

You can also interpret this as superposition of "oppositely charged pipes" (with a non-zero field going through the symmetry plane) and "both pipes with the same charge" (with zero orthogonal field at the symmetry plane).
 
Interesting. If two pipes have opposite charge however, the equipotential surfaces are exactly cylinders, which helps when using parallel pipes. However if they have the same charge, the surfaces are very distorted and do not form circles.

Do you know of a solution to two conducting pipes with potential of +V and +V?

Thanks for your help
 

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