Electric field and Laplace's equation

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Homework Help Overview

The discussion revolves around a problem involving the electric field generated by a conducting sheet shaped like a wedge, with a focus on applying Laplace's equation to find the relationship between the electric field magnitude and the radial distance from the bend.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore the use of separation of variables in cylindrical coordinates for solving Laplace's equation. Questions arise regarding the physical reasoning behind certain terms in the potential function and the implications of boundary conditions.

Discussion Status

The discussion is active, with participants providing insights into the mathematical approach and raising questions about the physical interpretation of the solution. Some guidance has been offered regarding the use of boundary conditions, though there is still uncertainty about which specific conditions apply.

Contextual Notes

There is mention of unspecified boundary conditions in the problem, leading to questions about their nature and how they relate to the behavior of potentials in the context of conductors.

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Homework Statement



I have to show for a conducting sheet bent along one axis into the shape of a wedge, with a certain angle, that the magnitude of the electric field in the bend is proportional to r^{(\pi/\theta) - 1}, where theta is the opening angle.


Homework Equations





The Attempt at a Solution



I'm not sure how to treat this problem, is this just separation of variables for Laplace's equation in three dimensions?
 
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You can use separation of variables for Laplace's equation in cylindrical coords. You also know the potential won't have any 'z' dependence so that will simplify your work.
 
I know what the solution is, but I don't really understand the physical logic behind it.

If V(s,\phi) = V_{0} + B_{0}Ln s + \Sigma (s^{n}[A cos (n\phi) + B sin (n\phi)] + s^{-n}[C cos (n\phi) + D sin (n\phi)])

Now, I know that at z = 0 this forces B_{0}, C, and D to go to zero (or else there will be infinite terms), but I don't understand necessarily why. What forces us to conclude, considering cylindrical symmetry, that s -> 0?
 
Don't forget you have boundary conditions you need to satisfy.
 
Okay, that's what I thought. But which boundary conditions are those if they are not specified in the problem?
 
They are specified in the problem. What do you know about potentials and conductors.
 

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