Voltage of an infinite cylinder with nontrivial reference point

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SUMMARY

The discussion focuses on calculating the electric potential V(r) due to an infinitely long cylinder with uniform charge density ρ and radius R, using V(r = 2R) = 0 as the reference point. The electric field equations are established as E at r < R = (ρr)/(2ε₀) and E at r > R = (ρR²)/(2ε₀r). The integration process for both regions is detailed, resulting in V(r < R) = (ρ/4ε₀)(4R² - r²) and V(r > R) = (ρR²)/(2ε₀)ln(2R/r). The calculations are confirmed to be correct based on the provided electric field equations.

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programmer1813
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Homework Statement


Find V(r), the electric potential due to an infinitely long cylinder with uniform charge density ρ and radius R.
Use V(r = 2R) = 0 as your reference point.

Homework Equations


E at r < R = ##\frac{(ρr)}{2ε_{0}}##
E at r > R = ##\frac{(ρR^{2})}{(2ε_{0}r)}##


The Attempt at a Solution


This is basically simple. Just integrate the electric fields to get voltage. The only problem is figuring out the limits of integration. I BELIEVE that if you have a nontrivial reference point outside of a cylinder, you will need to integrate from r to 2R for both inside and outside. So I did this:

$$V(r < R) = \int_r^R \frac{\rho r}{2ε_{0}}dr + \int_R^{2R} \frac{\rho r}{2\epsilon_{0}}dr = \frac{\rho}{4\epsilon_{0}}(4R^{2} - r^{2})$$

$$V(r > R) = \int_r^{2R} \frac{\rho R^{2}}{2\epsilon_{0}r}dr = \frac{\rho R^{2}}{2\epsilon_{0}}ln(\frac{2R}{r})$$

Does this look right?
 
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Assuming your field calculations are correct, these look right.
 
I'm not following the logic behind your equations.
For r > R, the field is ##E = \frac{\rho r}{2\pi\epsilon_0 R^2}##, yes?
So for r > R, isn't the potential ##\int_{s=r}^{2R}\frac{\rho s}{2\pi\epsilon_0 R^2}.ds##?
 

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