Electric Field at Surface & Inside Thin Hollow Sphere

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SUMMARY

The discussion focuses on calculating the electric field at the surface and inside a thin hollow sphere with a uniform surface charge density, denoted as 'a'. It is established that the magnitude of the electric field at the surface is |a|/E0, where E0 represents the permittivity of free space. Additionally, when a tiny hole is drilled through the sphere, the electric field in that hole is |a|/2E0. The calculations utilize Gauss' Law and the principle of superposition to derive these results.

PREREQUISITES
  • Understanding of Gauss' Law in electrostatics
  • Familiarity with electric field concepts and surface charge density
  • Knowledge of the permittivity of free space (E0)
  • Basic principles of superposition in electric fields
NEXT STEPS
  • Study the application of Gauss' Law in various geometries
  • Explore the concept of electric fields from infinite sheets of charge
  • Investigate the effects of surface charge density on electric fields
  • Learn about the implications of superposition in electrostatics
USEFUL FOR

This discussion is beneficial for physics students, educators, and anyone interested in understanding electrostatics, particularly the behavior of electric fields in charged spherical objects.

PinkFlamingo
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I'm also stuck on this one. Could someone help me please? :confused:

An insulating, thin, hollow sphere has a uniform surface charge density, a.

a) show that the magnitude of the electric field at the surface of the sphere is |a|/E0 (where E0 is the permittivity of free space)

b) a tiny hole is drilled through the shell, thus removing a negligible but of the charge. Show that the magnitude of the electric field in this hole is |a|/2E0
 
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For part a, consider that the surface of the Earth "looks" flat to us. Alternatively, you can use Gauss' Law and symmetry.

I'd have to think about b for a little bit. I'll leave that to one of the regular helpers here.
 
For Part b: The original sphere with a hole in it can be viewed as a superposition of the sphere with charge density a and the "hole" (i. e. a little piece of the surface) with charge density -a . So what you do is you compute the fields of the two charge distributions separately and then add them up. The field of the sphere you've computed already (zero inside!), and the field of a surface charge is...
 
If the point is sufficiently close to the surface of the sphere, then even the "little piece of surface" that kueng described looks like an infinite sheet of charge to that point...and the field from an infinite sheet of charge is...
 

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