Electric potential due to long wire

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Homework Statement


Using Gauss' law, or otherwise, find an expression for electric potential at a distance r from an infinitely long straight line of charge of length h with linear charge density lambda per unit length.

Homework Equations



q=lambda*h


The Attempt at a Solution


The first part is easy, using gauss' law to find electric field..the result i get is

E=lambda/(2*pi*r*epsilon_0)

..which should be correct. But then I'm not sure how to find potential in this case. I tried using the equation:

E= - grad*V

so

V = integral[E*dl]

V= -lambda/(2*pi*epsilon_0) integral_from_infinity_to_r[(1/r) dr]

..which leads me to:

V = -lambda/(2*pi*epsilon_0) [ln(r)]

where the ln(r) is evaluated from infinity to r...and I am not sure that looks right, or where to go from there.. :confused: I don't know what the solution is supposed to be and I couldn't find any explanations when i googled it..anyone have any idea? :rolleyes: thankyou sooo much!
 
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Hello.

In fact that's the solution. That's life!
 
heh :redface: thankyou!
 
how do you evaluate ln at infinity and r??
 
pick an arbitrary point a, and integrate with respect to that point. you're correct that you can't integrate to an infinite potential at the wire.
 
the only way i can think of is that u have to assume the boundary condition that V=0 at infinity. but then that seems forced because when evaluating the similar case for a sphere u get a 1/r term and when u plug in infinity there it goes to zero (see griffiths 3rd ed example 2.6). can anyone reconcile these cases? i don't see any explanation above addressing this.
 
Hi,

You cannot use infinity, because the problem states that there is an infinite length of wire. This tells us that the charge is infinite. Using a variable like "a" is your best bet for solving the problem.
 
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