Flux of a Cube with a Corner Charge

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SUMMARY

The net electric flux through all faces of a cube with a point charge located at one of its corners is calculated using Gauss's Law. The correct formula is φ = q/(8ε₀), where q is the charge and ε₀ is the permittivity of free space. This result arises because only one-eighth of the total flux from the charge contributes to the cube, as the electric field is parallel to three of the cube's faces, resulting in no flux through those faces. The symmetry of the arrangement confirms that the flux is evenly distributed among eight surrounding cubes.

PREREQUISITES
  • Understanding of Gauss's Law
  • Familiarity with electric flux concepts
  • Knowledge of permittivity of free space (ε₀)
  • Basic principles of symmetry in electrostatics
NEXT STEPS
  • Study advanced applications of Gauss's Law in different geometries
  • Explore electric field calculations for point charges
  • Learn about the concept of electric flux in various configurations
  • Investigate the implications of symmetry in electrostatic problems
USEFUL FOR

Students of electromagnetism, physics educators, and anyone interested in understanding electric flux and its applications in electrostatics.

breez
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Homework Statement



A point charge is placed at a corner of a cube. What is the net flux through all faces of the cube?

Homework Equations





The Attempt at a Solution



\phi = \frac{q}{\epsilon_0}

or perhaps

\phi = \frac{q}{8\epsilon_0}

The latter solution is based on the fact that for 3 faces on the cube, no flux will be present as the e field is parallel to the faces. Place 7 other cubes about this cube to force a cube with the charge in the middle, and each cube individually will only have flux through 3 of the cubes. A charge enclosed in a gaussian surface must result in a flux of \phi = \frac{q}{\epsilon_0} for the surface. There are 8 cubes, and our original situation is 1/8 of the entire cube, and hence: \phi = \frac{q}{8\epsilon_0}
 
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breez said:

The Attempt at a Solution



\phi = \frac{q}{\epsilon_0}
That's the total flux from the point charge.

or perhaps

\phi = \frac{q}{8\epsilon_0}
That's the one you want.

The latter solution is based on the fact that for 3 faces on the cube, no flux will be present as the e field is parallel to the faces. Place 7 other cubes about this cube to force a cube with the charge in the middle, and each cube individually will only have flux through 3 of the cubes. A charge enclosed in a gaussian surface must result in a flux of \phi = \frac{q}{\epsilon_0} for the surface. There are 8 cubes, and our original situation is 1/8 of the entire cube, and hence: \phi = \frac{q}{8\epsilon_0}
Sounds good. I'd view it as a 2x2x2 stack of 8 cubes with the charge at the center corner. By symmetry, the flux is equally distributed among the 8 cubes. Done!
 

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