Electric potential of cylinder problem

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SUMMARY

The discussion focuses on calculating the electric potential of a solid cylinder with uniform charge density (ρ) at a point P located on the z-axis outside the cylinder. Participants suggest using integration techniques similar to those applied for a uniformly charged disk, dividing the cylinder into stacked disks for potential contributions. The conversation also touches on the application of Gauss's Law and the importance of cylindrical symmetry when determining electric fields and potentials. Key references include Griffiths' "Introduction to Electrodynamics" for relevant equations.

PREREQUISITES
  • Understanding of electrostatics, specifically electric potential and electric fields.
  • Familiarity with Gauss's Law and its application to cylindrical symmetry.
  • Knowledge of integration techniques for calculating potential from charge distributions.
  • Basic concepts of electrostatic potential energy (U) versus electric potential (V).
NEXT STEPS
  • Study the derivation of electric potential from charge density using Griffiths' equations, particularly equation 2.29.
  • Learn about the implications of finite versus infinite cylindrical charge distributions on electric field calculations.
  • Explore advanced integration techniques for potential calculations in electrostatics.
  • Review the differences between electrostatic potential energy and electric potential in detail.
USEFUL FOR

Students and educators in physics, particularly those focusing on electromagnetism, as well as anyone involved in solving electrostatic problems related to charged cylinders.

azone
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Homework Statement



A solid cylinder with radius R and length L has uniform charge density ro. Its base is in the x-y plane and it's axis is coincident with the z-axis (symmetrical about the z-axis)

Homework Equations



Find the electric potential at point P outside the cylinder at a distance z from the origin (P is on the z-axis)

The Attempt at a Solution



So I compared this to finding the potential at a distance z above a uniformly charged disk. In the case of a disk, I divided the disk into concentric rings, found the potential contribution due to one ring, and then integrated over all rings with the limits 0 to R.
I tried to use a similar argument and divide the cylinder into equal sized disks with radius R stacked on top of one another (so the only difference is the distance from the point P). I then want to integrate this over all disks with the limits 0 to z. So can I just use my answer for the potential above a charged disk, and then integrate it with respect to z to cover all the distances?
thanks!
 
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You idea sounds correct.
 
hi i have the same proplem but for height 2h and radius (a) and charge density ro inside and outside the cylinder and i tryed to use gauss's law and find fy the electric potential but I'm not sure can some one help.
i use
V(r)=- integrate E.da=E.2pi a (2h) =1/ebslon .Qenc
 
I would use Gauss's Law to find the E-vectors around and inside the cylinder, when remember that U=\int_{\infty}^r \vec{E}\bullet d\vec{l} and V=\frac{U}{q}.

A hint: Use a cylinder for your gaussian surface, with the same axis as your charged cylinder.
 
Thanks, but what you mean by U, is it the electric potential ?
I'm convusing between the notations !
 
Hi eman2009, I think espen180 is confusing electrostatic potential energy and electrostatic potential.

As for your original question, if the cylinder only has a finite length 2h, does it still have the requisite cylindrical symmetry to use Gauss' Law?

If not, you'll have to find the potential through another means...can you think of any formulas that directly relate potential to charge density?
 
how about

close INT E . da=1/ebsolon Qenc

as in Griffiths book(Introduction to Electrodynamic) p.68, equation 2.13
and
Q=INT RO dt t(tao) is the infinitesimal displacement

dt for cylinder

dt=4 pi R^2 dr
 
That's just Gauss' Law, and it is only useful in cases where symmetry allows you to pull E outside of the integral...is a cylinder of finite length one of those cases?

Instead, try equation 2.29, it directly relates rho to V.
 
eman2009 said:
Thanks, but what you mean by U, is it the electric potential ?
I'm convusing between the notations !

Sorry, I mistook your cylinder as one of infinite length. As for my notation, U is the electrostatic potential energy and V is the electric potential.
 
  • #10
espen180 said:
Sorry, I mistook your cylinder as one of infinite length. As for my notation, U is the electrostatic potential energy and V is the electric potential.

Sure, but wouldn't you also say

U(r)=-\int_{\infty}^r \vec{F}\bullet d\vec{l}\neq\int_{\infty}^r \vec{E}\bullet d\vec{l}

?:wink:
 
  • #11
Gah! You're right! Sorry about that. It should be an F, not an E.
 

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