Gauss's Law: Solve Cylindrical Shell Problem

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Homework Help Overview

The problem involves a cylindrical shell with a uniform charge distribution on its surface. The task is to determine the net charge on the shell and the electric field at a specific point inside the shell, given the electric field at a point outside the shell.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to understand why the distance used in calculations for the electric field outside the shell is 19 cm instead of 12 cm, questioning the implications of charge distribution and the electric field inside the shell.
  • Some participants discuss the relationship between charge density, area, and electric field strength, suggesting that the field effect from the charge decreases with distance.
  • There is a consideration of whether the cylindrical shell can be approximated as a line charge due to similarities in their equations.

Discussion Status

The discussion is ongoing, with participants exploring the implications of Gauss's law and the nature of electric fields in relation to cylindrical shells. Some guidance has been offered regarding the application of Gauss's law to closed surfaces, but no consensus has been reached on the original poster's specific confusion.

Contextual Notes

Participants are navigating the assumptions about charge distribution and the behavior of electric fields in relation to cylindrical geometries, with some uncertainty about the implications of these assumptions on the calculations being performed.

jghlee
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Homework Statement


So here's the question...

A cylindrical shell of radius 7.00 cm and length 240 cm has its charge uniformly distributed on its curved surface. The magnitude of the electric field at a point 19.0 cm radially outward from its axis (mesaured from the midpoint of the shell) is 36.0 kN/C. Find (a) the net charge on the shell and (b) the electric field at a point 4.00 cm from the axis, measured radially outward from the midpoint of the shell.

Homework Equations


Flux = EA = q/Eo

The Attempt at a Solution


I was able to get the answer at (a) but I'm seriously questioning myself after taking a look at (b). So, basically (b) states that the E inside the cylindrical shell is 0 since all the charges reside on the surface of the spherical shell (so there's no charge inside right?). I solved (a) by ...
(3.6e4)(2r(pi)x) = q/Eo... where x=19cm since that's the distance from the center of the cylindrical shell to the point at where the E is 36.0 KN/c.

So that's the right way to do it but here's what confuses me. Why do we use 19cm instead of (19-7=12cm) when there are no charges inside the cylindrical shell? Isn't the charges ONLY coming from the surface of the shell? So basically shouldn't the distance from the charge to the point where we find the E be 12cm?

Any help will be appreciated :D
 
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You are correct there is no charge inside the shell.
Why do we use 19cm instead of (19-7=12cm) when there are no charges inside the cylindrical shell?
Consider the area of the cylindrical surface. It increases with r2.

So charge density decreases with area. (Q/A) And so does the field effect from the charge decrease with 1/r2.

So whether it is a line charge with 0 radius but charge measured by unit length, or surface charge at some radius, the field effect at some radial distance from the axis and outside the surface will be the same.

Line charge:
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elecyl.html#c1
conducting cylinder:
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elecyl.html#c2
 
So, just to make sure I'm on the right page here, we can basically consider the conducting cylinder as a really thick line charge?
 
jghlee said:
So, just to make sure I'm on the right page here, we can basically consider the conducting cylinder as a really thick line charge?

Well the equations certainly bear a remarkable similarity don't they?
 
thanks for the help LowlyPion
 
Gauss' law:

[tex]\oint_S \mathbf{E} \cdot \mathrm{d}\mathbf{A} = \frac{Q_{\mathrm{enclosed}}}{\varepsilon_0}[/tex]

applies to any closed surface whatsoever. That means you don't need to care how the charges are distributed inside the surface; as long as you have a closed surface, like the surface of a sphere, cylinder, or cube, the equation holds.
 

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