Find the electrostatic potential due to a hoop of charge

Click For Summary
SUMMARY

The discussion focuses on calculating the electrostatic potential due to a hoop of charge with radius k, centered on the x-axis. The linear charge density is denoted as j, and the potential Fi at points on the x-axis is derived as Fi(x, 0, 0) = (2*pi*j)/|x| for points far from the hoop. The solution involves integrating the charge elements and applying symmetry principles, leading to the conclusion that the potential behaves inversely with distance from the hoop.

PREREQUISITES
  • Understanding of electrostatics and potential theory
  • Familiarity with integration techniques in calculus
  • Knowledge of symmetry in physical systems
  • Basic concepts of charge density and electric fields
NEXT STEPS
  • Study the derivation of electric potential from electric fields using integration techniques
  • Learn about the application of symmetry in electrostatics problems
  • Explore the concept of equipotential surfaces and their significance in electrostatics
  • Investigate the behavior of electric fields and potentials in different geometries, such as spherical and cylindrical distributions
USEFUL FOR

Students and professionals in physics, particularly those focusing on electrostatics, as well as educators looking for examples of charge distribution problems and their solutions.

wam_mi
Messages
78
Reaction score
1

Homework Statement



(Part 1) A hoop of charge of radius k lies in the y, z plane, centred on the x axis, so that
it occupies the points (0, y, z) with y^2 + z^2 = k^2. If the (linear) charge density
in the hoop is j, calculate the electrostatic potential Fi at all points on the
x axis, and show that, far from the hoop on the x axis, Fi (x, 0, 0) = (2*pi*j)/|x|.
Explain briefly why this result was only to be expected.

(Part 2) More generally, what do you expect the leading behaviour of Fi(r) to be, far
from the hoop? (You do not need to give any detailed calculations.) Use your
answer to deduce the limiting forms of the equipotential surfaces and field lines,
again far from the hoop.


Homework Equations




The Attempt at a Solution



(Part 1)

Total Charge Q = Integrating j * dl with interval [0 , 2*pi]
= 2*pi*k*j

By Symmetry, Fi (x) = 2*pi*k*j / |x| (Is this wrong?)

And now I'm stuck for the rest of the question.

Please help! Thank you!
 
Physics news on Phys.org
Integrating the charge elements and using symmetry is involved for solving this problem.

[tex]E = E_x =\int\mbox{dEcos}\theta\mbox{d}\theta[/tex]

where

[tex]dE =\frac{Kd\rho}{r^2}[/tex]

The sine components of E cancel due to symmetry, and

[tex]cos\theta = \frac{x}{\sqrt{k^2+x^2}}[/tex]

The charge element is

[tex]d\rho = jkd\phi \ \mbox{and}\ d\phi \ \mbox{ is integrated from 0 to} \ 2\pi[/tex]

Once E is found, the potential is found from integrating E from infinity to x along the x axis.
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
5K
  • · Replies 19 ·
Replies
19
Views
3K
Replies
19
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 13 ·
Replies
13
Views
6K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 6 ·
Replies
6
Views
3K