Using a cube as a Gaussian surface

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SUMMARY

The discussion centers on the practicality of using a Gaussian surface in the shape of a cube to compute the electric field (E field) outside a uniformly charged cube. The larger cube, with double the side length, is symmetrical to the smaller cube. While Gauss' Law can be applied, the complexity arises due to the cancellation of electric field lines from the inner cube, leading to a discontinuous E field. The proposed solution involves simplifying the inner charged cube to a point charge, which complicates the integration process due to the angles between the electric field vector and the area vector of the Gaussian surface.

PREREQUISITES
  • Understanding of Gauss' Law and its mathematical formulation
  • Familiarity with electric field concepts and vector calculus
  • Knowledge of symmetry in electric fields and charge distributions
  • Experience with integration techniques in three-dimensional space
NEXT STEPS
  • Study advanced applications of Gauss' Law in non-spherical geometries
  • Learn about electric field calculations for various charge distributions
  • Explore vector calculus techniques for integrating over complex geometries
  • Investigate numerical methods for approximating electric fields in irregular shapes
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Physics students, electrical engineers, and anyone interested in electrostatics and the application of Gauss' Law in complex geometrical configurations.

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Homework Statement



Suppose there is a uniformly charged cube with known side length. I then imagine a larger, closed cube surface surrounding it. This larger cube has double the side length and is symmetrical to the smaller cube.

Is is practical to use this Gaussian surface to compute the value of the E field at some arbitrary point outside the charged cube?

Homework Equations


Gauss' Law, \intE*da = q/\epsilon


The Attempt at a Solution



A classmate told me that this would be very difficult to do, and that no, using a cubical Gaussian surface would not work very well in a practical sense.

When I think of this problem, this is what I think:
Every charge on the surface of the inner cube will have an electric field pointing away from its center radially. Since the cube is symmetrical, though, many of these field lines will cancel each other out, leaving only field lines going outward from the inner cube perpendicular to each cube face. That would mean that the larger, imaginary cube would experience a flux out of each of its cube faces equal to the E field coming from each inner cube face. The sum of each face would then allow us to know the total flux leaving the Gaussian surface.

However, this would give us a discontinuous E field, one that would have no flux or E field coming off the edges. This would give us E field lines in a 3D cross shape.

I have no clue if this problem is very simple or very difficult. Any insights are very warmly welcome.
 
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One more idea for solving this:

If I simplify the the inner charged cube to just be a point charge surrounded by a cubical Gaussian surface, then computing the E field is very difficult. It is not simple because the electric field vector coming from the charge is often at an angle to the area vector of the imaginary surface. It would be a very difficult integral to execute.
 
I don't see how Gauss can help here.

I would orient the cube with its center at (0,0,0) and observation point along the x axis, then compute the potential by integration and finally take the negative gradient of that potential. At least that way you only have to integrate over 1/4th the cube volume.
 

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