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- Thread starter scrappy
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No, you have to use Coulomb's law.can we use gauss' law to find the e field of a finite line of charge?

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thank you for the response sir.

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Well, I'll wait and see if anyone posts a way to do it. If you find a way on your own, please post it. I'd like to learn if there is a way.

thank you for the response sir.

There is one sense in which you can do it. Since Gauss's Law basically contains Coulomb's Law in it, you can argue that the use of Coulomb's law is essentially the same as using Gauss' Law. However, I don't see any way to use Guass's law directly on a finite length of charge because there is not enough symmetry to get an exact solution this way. You can do it for an infinite length of charge.

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anyway, thank you so much for your help sir. i wish someone could tell us how to.

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Gauss's law is a law, so it will always "work." For a finite line of charge, it is just not useful.

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are there any solutions online using gauss law to solve this? if anybody knows, please inform me. your help will be very much appreciated. ^_^

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The following reference contains the derivation of several charge distributions including the finite line of charge. Here they use Coulomb's Law, which is the way most people approach solving this problem.

are there any solutions online using gauss law to solve this? if anybody knows, please inform me. your help will be very much appreciated. ^_^

http://iweb.tntech.edu/murdock/books/v4chap2.pdf

Note that it is trivial to derive Coulomb's Law directly from Gauss' Law by applying it to a point charge using spherical symmetry. It is also possible to derive Gauss' Law from Coulomb's Law, although this is not quite as easy to do. For example, see Jackson's well known EM book for a very elegant derivation; or, Schwartz provides a step by step mathematical derivation.

So, it seems to me that applying Coulomb's Law is an acceptable way to solve the given problem. First derive Coulomb's Law from Gauss' Law, and then apply Coulomb's Law to the given problem using integration and the principle of superposition.

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