Electric Field over a charged cylinder using only Coulomb's Law

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Homework Help Overview

The problem involves determining the electric field at a point on the central axis of a solid, uniformly charged cylinder using Coulomb's Law. The original poster presents an integral setup for calculating the electric field but encounters difficulties with the integration process and the resulting expressions.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to evaluate a triple integral to find the electric field, but questions arise regarding the assumptions made in the integrand. Some participants suggest re-evaluating specific terms in the expression, particularly concerning the treatment of absolute values.

Discussion Status

The discussion is ongoing, with participants exploring the implications of the integral setup and the resulting logarithmic terms. There is a recognition of the complexity involved in integrating the absolute value function, and some guidance has been offered regarding the assumptions made in the calculations.

Contextual Notes

Participants are working under the constraints of using Coulomb's Law and are focused on the mathematical intricacies of the integration process. There is an acknowledgment of potential errors in the setup and assumptions that may affect the outcome.

PeteyCoco
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Homework Statement



What is the electric field at a point on the central axis of a solid, uniformly charged cylinder of radis R and length h?

Homework Equations



Well, I've set up the triple integral and have gotten to this point:

[itex]\bar{E}_{z}=\frac{2\pi\rho}{4\pi\epsilon_{0}}\int^{h/2}_{-h/2}[1-\frac{z'-z}{\sqrt{(z'-z)^{2}+R^{2}}}]dz[/itex] , z' is the location of the test point

When I integrate this I get a constant term and a mess of logarithms. I know that the field should be 0 when z' = 0, but it doesn't check out. What's wrong?
 
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PeteyCoco said:
Well, I've set up the triple integral and have gotten to this point:

[itex]\bar{E}_{z}=\frac{2\pi\rho}{4\pi\epsilon_{0}}\int^{h/2}_{-h/2}[1-\frac{z'-z}{\sqrt{(z'-z)^{2}+R^{2}}}]dz[/itex]

Re-evaluate how you got the 1 inside the brackets in the expression above. I suspect that you got this from assuming that ##\frac{z'-z}{\sqrt{(z'-z)^2}} = 1##. But, recall that ##\sqrt{x^2} = |x|##.
 
Alright. Now that I've changed that term, it vanishes when integrated, but the second term in the integrand still turns into

[itex]\frac{1}{2}ln| (z'-z) + \sqrt{(z'-z)^{2}+R^{2}} |^{h/2}_{-h/2}[/itex]

Which, as far as I can tell, can't be reduced to 0 when z' = 0
 
Nevermind, integrating this absolute value function is a bit more work than I thought it was.
 
Also, I don't see how you are getting a logarithm expression in the result of the integration.
 

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