Integral from an electric field calculation

AI Thread Summary
The integral presented is crucial for calculating the electric field of a uniformly charged spherical shell. The specific integral is $$ \int_{0}^{\pi} \frac{(z-R\cos{\theta})\sin{\theta}d\theta}{R^2+z^2-2ZR\cos{\theta}}$$, where the variable z represents the distance from the center of the shell. When z equals R, the result aligns with the expected electric field of an infinite plane, given by $$ E_z=\sigma/2\epsilon_0 $$. The discussion seeks methods for solving this integral to further understand the electric field behavior. Overall, the integral plays a significant role in electrostatics related to spherical charge distributions.
klawlor419
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Hi all,

Any ideas how to solve this integral?

$$ \int_{0}^{\pi} \frac{(z-R\cos{\theta})\sin{\theta}d\theta}{R^2+z^2-2zr\cos{\theta}}$$

It crops up in a calculation of the electric field for a spherical charged shell. It has a uniform charge smear

Thanks ahead of time
 
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The lower case r in the denominator should be a large R for the radius of the shell.
 
Well, I figured out that when z=R you recover the expected field of an infinite plane.

$$ E_z=\sigma/2\epsilon_0 $$
 
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