Surface Charge Density of a Neutral Conducting Cube

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SUMMARY

The discussion focuses on calculating the surface charge density of a neutral conducting cube placed in a uniform electric field E. Using Gauss' Law, it is established that only the faces III and VI of the cube will have a non-zero surface charge density, while faces I, II, IV, and V will have zero charge density due to their orientation relative to the electric field. The surface charge density η is derived as η = Eε₀, where ε₀ is the permittivity of free space. This conclusion is reached by analyzing the electric flux through the cube's surfaces and applying the relevant equations.

PREREQUISITES
  • Understanding of Gauss' Law and its application in electrostatics.
  • Familiarity with electric flux and surface charge density concepts.
  • Knowledge of vector calculus, particularly in relation to area vectors and angles.
  • Basic principles of conductors in electrostatic equilibrium.
NEXT STEPS
  • Study the implications of Gauss' Law in different geometries, such as spheres and cylinders.
  • Learn about the behavior of electric fields in conductors and insulators.
  • Explore the concept of electric displacement field and its relation to surface charge density.
  • Investigate advanced applications of electrostatics in real-world scenarios, such as capacitors and shielding.
USEFUL FOR

This discussion is beneficial for physics students, electrical engineers, and anyone interested in understanding electrostatics and the behavior of conductors in electric fields.

inevitable08
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Homework Statement


There is a region of space containing a uniform electric field of strength E. A neutral conducting cube with side length s is placed into this field. The cube is aligned with the field. You may assume that the electric field outside the cube is unaffected by any changes that occur in the cube. Use Gauss’ Law and your knowledge of conductors to find the surface charge density, if any, on each face of the cube. Your results may be in terms of E, s, and any appropriate constants. The three visible cube faces are numbered, I, II, and III. Assume that face IV is opposite face I, face V is opposite face II, and face VI is opposite face II.


Homework Equations


Electric Flux = E (dot) A = EAcosθ = Qencl/\epsilon_{o}\
η = surface charge density of a plane of charge = q/area

The Attempt at a Solution


Ok since we are dealing with a cube this means the surface is flat and the charge density is not changing so we don't need to integrate A for surface. I also know that any area vectors of the cube that are orthogonal with the electric field creates an electric flux of 0. This means sides I, II, IV, and V are all going to be 0 this now leaves us with III and VI.

III's area vector is in same direction as the field so this means cos(θ) = 1 and VI is opposite and cos(θ) = -1.

A(q/A) = Aη = Qencl

plug in information

EA = Qencl/\epsilon_{o}\

EA = Aη/\epsilon_{o}\

E\epsilon_{o}\ = η


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I just feel this can't be right, seems to simple
 

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It is inevitably :smile: correct.

ehild
 

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