Electric field and Laplace's equation

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SUMMARY

The discussion focuses on solving a problem involving a conducting sheet bent into a wedge shape, specifically determining the electric field's magnitude in the bend as proportional to r^{(\pi/\theta) - 1}, where theta represents the opening angle. The solution involves applying Laplace's equation in cylindrical coordinates, utilizing separation of variables. Key insights include the elimination of 'z' dependence in the potential function and the necessity of satisfying boundary conditions related to conductors. The participants emphasize the importance of understanding these boundary conditions to derive the correct electric field behavior.

PREREQUISITES
  • Understanding of Laplace's equation in cylindrical coordinates
  • Knowledge of electric potential and its relation to electric fields
  • Familiarity with boundary conditions in electrostatics
  • Concept of cylindrical symmetry in physical problems
NEXT STEPS
  • Study the application of separation of variables in solving Laplace's equation
  • Explore the relationship between electric potential and electric field in electrostatics
  • Research boundary conditions for conductors in electrostatic problems
  • Learn about cylindrical coordinate systems and their applications in physics
USEFUL FOR

Students and professionals in physics, particularly those focusing on electrostatics, electrical engineering, and mathematical methods in physics. This discussion is beneficial for anyone looking to deepen their understanding of electric fields and potential in complex geometries.

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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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