How Should I Integrate Electric Potential for Oppositely Charged Parallel Lines?

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SUMMARY

The discussion focuses on integrating electric potential for two infinite parallel lines of charge with charge densities +λ and -λ located at x = a and x = -a, respectively. The user, W, seeks clarification on the correct limits of integration when calculating the potential at a point r, particularly addressing the issue of integrating from -a to r, which leads to the natural logarithm of a negative number. The correct approach involves using the absolute distances |x + a| and |x - a| to ensure positive values in the integration process.

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wakko101
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electric potential...again.

So, I've still got my two infinite lines of charge that run parallel to the x-axis running along the lines x = a and x = -a and with charge density + and - lambda respectively.

I've figured out that using the origin as my reference point allows me to integrate the electric field of my lines from a to the point in question (r). However, because the field goes like 1/r, we end up with a ln of something in the potential. For the line that's positive a away from the x axis, there's no problem. But, for the line that runs along x = -a, how can I integrate? should I be integrating from a to r again, or from -a to r. The problem with the latter is that you can't have the natural logarithm of a negative number.

I would REALLY appreciate any advice. I'm a little desperate...

Cheers,
W. =)
 
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Remember, the r in 1/r is the distance to the charge so it should always be positive. If your point is (x, y) then the distance to the line x = -a is |x + a| and the distance to the line x=a is |x-a|
 
that makes sense...I figured it was a that I needed to use, but I just wanted to be sure.

Thanks for the help. =)
 

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