What Are the Limits for Calculating the Radial Electric Field Potential?

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SUMMARY

The discussion focuses on calculating the radial electric field potential due to a point charge 'q' using the formula E = (1 / 4∏ε) * (q/r^2). The potential difference ΔV is derived by integrating the electric field along a radial path from infinity to a distance r2, resulting in ΔV = - (q/4∏ε) ∫(1/r^2) dr. The correct limits for the integral are confirmed to be from infinity to r2, with V(∞) set to zero.

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chris_avfc
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Homework Statement



Radial component of an electric field near charge 'q'.

E = (1 / 4∏ε) * (q/r^2)

Need to find the potential of this which is done through integrating this and taking the negative answer, i.e.

ΔV = -∫E dr

This is to be along a radial path towards the charge, starting from infinity to r2.


The Attempt at a Solution



So I have

ΔV = - (q/4∏ε) ∫1/r^2 dr

As the charge is constant.
Just unsure on the limits, I'm guessing its ∞ and r2, would that be right?
 
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[tex]\Delta V=V(r)-V(\infty)=-\frac{q}{4\pi \epsilon _0}\int_{\infty}^r{\frac{1}{r^2}dr}[/tex],

with V(∞)=0


ehild
 
ehild said:
[tex]\Delta V=V(r)-V(\infty)=-\frac{q}{4\pi \epsilon _0}\int_{\infty}^r{\frac{1}{r^2}dr}[/tex],

with V(∞)=0


ehild

Awesome, cheers mate. I had my limits the wrong way around.
 

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