Gauss' Law and an infinite sheet

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Homework Help Overview

The problem involves calculating the electric field at a point above a nonconducting infinite sheet with a circular hole, given a uniform charge density. The context is rooted in Gauss' Law and the principles of superposition in electrostatics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of superposition to find the electric field due to both the infinite sheet and the hole. There is uncertainty about how to combine the effects of the sheet and the hole, particularly regarding the signs of the charge densities involved.

Discussion Status

Some participants have suggested using the electric field equations for both the infinite sheet and the disk representing the hole. There is acknowledgment of the need to consider the opposite sign for the hole's charge density, and a general agreement on the approach to combine the two fields.

Contextual Notes

Participants note the importance of the hint regarding superposition and the specific equations related to the electric fields of the sheet and the disk. There is a mention of the lack of a figure being a potential source of confusion.

catie1981
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Homework Statement



a small circular hole of radius R = 2.03 cm has been cut in the middle of an infinite, flat, nonconducting surface that has a uniform charge density σ = 4.61 pC/m^2. A z axis, with its origin at the hole's center, is perpendicular to the surface. What is the magnitude (in N/C) of the electric field at point P at z = 3.05 cm? (Hint: See Eq. 22-26 and use superposition.)

There is supposed to be a figure, but it really doesn't lend much to this. It is a flat sheet laid on the horizon, with the z axis going through a hole in the middle of the sheet. Point P is on the z axis, and R is just shown as the radius of the hole in the sheet. Which, is pretty much what was said in the problem...

Homework Equations



the equation mentioned above is
E = (σ / 2ε) *( 1- z/ (√z^2 + R^2))

but how I'm supposed to use that and superposition, I am not sure.


The Attempt at a Solution


I want to just plug in the given values, but I don't think that it right, because the question mentions superposition, but what am I adding together?! There was an additional hint about using a disc of equal magnitude and such, but oppostire direction. Wouldn't I then need a different equation? Help! (and Thanks)
 
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There is a favorite trick for dealing with "holes" in charge distributions. You use the superposition of the field for an infinite sheet of uniform surface charge density σ , together with the field for a disk the size of the "hole", having uniform surface charge density -σ .
 
oooo, so for the sheet I would use sigma/2*epsilon and the disc would have a -sigma value...then I add those numbers and viola! I have the solution. Thanks!
 
catie1981 said:
oooo, so for the sheet I would use sigma/2*epsilon

Yes, for its electric field, since this is a non-conducting sheet.

and the disc would have a -sigma value...

Yes, in the equation you were given for the field along the axis for a uniformly charged disk at a distance z from the plane of the disk.

then I add those numbers and viola!

That should do it.
 

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