Electric potential along the axis of a cylindric tube

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SUMMARY

The discussion focuses on calculating the electric potential along the axis of a cylindrical tube with a uniform surface charge density (σ). The solution involves treating the cylinder as a series of stacked line charges (rings) and integrating the electric potential contributions from each ring. The key steps include determining the axial electric field (dE) from a ring of charge and recognizing that dE has only an axial component due to symmetry. Participants are encouraged to set up the integral for further assistance.

PREREQUISITES
  • Understanding of electric potential and electric fields
  • Familiarity with integration techniques in calculus
  • Knowledge of cylindrical coordinates
  • Concept of surface charge density (σ)
NEXT STEPS
  • Study the derivation of electric potential from line charges
  • Learn how to set up and evaluate integrals in cylindrical coordinates
  • Explore the relationship between electric potential and electric field
  • Investigate symmetry in electrostatics and its implications on electric fields
USEFUL FOR

Students studying electromagnetism, physics educators, and anyone interested in advanced electrostatics concepts.

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Homework Statement


Imagine a cylinder of radius R and Length L. Both of it's ends are open and it carries a uniform surface charge desnity of sigma (@) Find the electric potential at any point along the axis of the cylinder, and then use that to calculate the electric field at any point.


Homework Equations





The Attempt at a Solution


Essentially the way you are supposed to do this problem (I think) is to assume the tube is just a bunch of stacked line charges (rings), and then find the potential from a ring, and then integrate from 0 to L or something, I'm having real trouble doing so however, any help out there?
Thanks
 
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Your concept is correct. Find dE for a ring line of charge and keep in mind dE has only an axial component due to symmetry. Try setting up the intergral and post it.
 

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