Electric Field from Long Hollow Cylinder

FS98
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Homework Statement



Consider the hollow cylinder from Exercise 1.59. Use Gauss’s law to show that the field inside the pipe is zero. Also show that the field outside is the same as if the charge were all on the axis. Is either statement true for a pipe of square cross section on which the charge is distributed with uniform surface density?

The cylinder is long.

Homework Equations



292a4114ec9c495a97f151c19fbcf4cf3f533194


9810529d253a8cc85469e17185424ea235655087
25px-OiintLaTeX.svg.png
3b570ea85ff659c8b20a3b538b0000c21c530162
6725e7a0cdea9f4dd1d9cd9ccf6df16e23164ba2


The Attempt at a Solution


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I have no idea how to do this problem. Can somebody walk me through it? I’m assuming I have to use the second equation here, but I’m not quite sure what some of it means or how to apply it.
 

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If you take a moment to reflect on what exactly Gauss' Law says, and in particular what Q is defined to be, then you should be able to make a good attempt at solution, if not solve the problem entirely.
 
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gneill said:
If you take a moment to reflect on what exactly Gauss' Law says, and in particular what Q is defined to be, then you should be able to make a good attempt at solution, if not solve the problem entirely.

Can I get phi by multiplying the volume of the cylinder by ρ then dividing by e0 to get pi(r^2)(h)(ρ)/e0?

Then do I plug that into the other formula? If so how? I don’t know what the double integral is and I’m unsure what to do with the da. Is that a dot product or is the da just letting you know what to integrate with respect to?
 
Last edited:
The double integral represents a surface integral, that is, over the Gaussian Surface. As such it's an integration over an area, hence the dA represents a differential "patch" of that surface area.

Take a look at the following PDF to review: http://bolvan.ph.utexas.edu/~vadim/classes/15s/GaussLaw.pdf
In one section it considers a hollow cylinder.

You need to choose suitable Gaussian surfaces (presumably taking advantage of the symmetry inherent in the scenario) that will allow you to evaluate the integral easily (essentially by inspection).
 

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