Electric field at (0,0) for this charged square conductor

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Homework Help Overview

The discussion revolves around determining the electric field at the center of a square charged conductor, specifically at the point (0,0). Participants explore the implications of symmetry in electric fields and the application of Gauss's law in this context.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants question whether the square charge can be treated similarly to a spherical shell regarding electric field calculations. There are discussions about the validity of assuming the electric field is zero based on symmetry and the challenges of applying Gauss's law due to the lack of symmetry in the square charge distribution.

Discussion Status

Some participants are exploring the symmetry of the electric field at the center of the square and how it affects the calculations. There are suggestions to visualize the electric field vectors and consider their cancellation. Guidance has been offered regarding the use of symmetry in equations without needing to perform complex integrals.

Contextual Notes

Participants express uncertainty about the necessity of calculations versus visual explanations, indicating a need for clarity on how to approach the problem effectively. There is also mention of the limitations of Gauss's law in this scenario due to the shape of the charge distribution.

requied
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Homework Statement
If this figure below is a conductor, what will be the electric field at (0,0) for the square charge distribution
Relevant Equations
Gauss' Law
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Can we assume that square charge resembles a sphere shell, and think like electric field at sphere shell's center is 0.
 
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This solution is true ? According to this,the electric field is 0 on anyplace in the square conductor.
 
No this solution is not correct. You can't take the E out of the integral, as you do in the 2nd line, because the spherical gaussian surface is not symmetrical with respect to the square charge density.
 
You are only asked for the field at (0,0). Isn't the answer obvious by symmetry?
 
haruspex said:
You are only asked for the field at (0,0). Isn't the answer obvious by symmetry?
Yeah it is obvious but I must attach an explain and show the calculations. Have you any offer to do it by this way? Or maybe a figure which can explain.
 
Delta2 said:
You can't take the E out of the integral, as you do in the 2nd line, because the spherical gaussian surface is not symmetrical with respect to the square charge density.
I have a trouble with square shape symmetry. How can I come through of it? Or maybe I don't have to show calculations, just draw a figure which can explain the logic.
 
requied said:
I have a trouble with square shape symmetry. How can I come through of it? Or maybe I don't have to show calculations, just draw a figure which can explain the logic.
Well the truth is that this square shaped charge density doesn't offer us with any symmetry that would be useful in Gauss's law. You just can't use Gauss's law (with any possible gaussian surface) to solve for the electric field in the interior.

However the point (0,0) has a special symmetry. To see this symmetry , try to draw the electric field vectors at the center due to each of the 4 sides of the square. You ll draw 4 vectors and then you ll have to argue how they cancel out in pairs. And then you ll conclude that the E-field at the center is indeed zero.
 
Delta2 said:
try to draw the electric field vectors at the center due to each of the 4 sides of the square. You ll draw 4 vectors and then you ll have to argue how they cancel out in pairs.
I've been thinking the same thing from the beginning. I'll solve this by this way, I hope it works for getting some point :) Thank you for attention.
 
requied said:
Yeah it is obvious but I must attach an explain and show the calculations. Have you any offer to do it by this way? Or maybe a figure which can explain.
You can use the symmetry in your equations. There is no need to solve any integral. Just write the integrals down and collect up terms that cancel.
 

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