Calculating Energy of Coaxial Cylinders

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SUMMARY

The discussion focuses on calculating the energy per unit length of two coaxial insulating cylinders with charge densities λ and -λ. The energy is derived using two methods: the integral of the electric field squared and the work done by the electric field. The electric field between the cylinders is determined using Gauss's law, yielding E = λ/(2πε0s). The potential difference is calculated as V = -∫E ds, leading to V = (λ/(2πε0)) * ln(b/a). The user clarifies the relationship between linear charge density and surface charge density, ultimately seeking confirmation on the limits of integration for their calculations.

PREREQUISITES
  • Understanding of Gauss's Law and its application to cylindrical symmetry
  • Familiarity with electric fields and potential energy concepts
  • Knowledge of integral calculus for evaluating work and energy
  • Basic understanding of charge density types: linear and surface charge density
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  • Review the derivation of electric fields using Gauss's Law for cylindrical geometries
  • Study the relationship between linear charge density and surface charge density in electrostatics
  • Learn how to calculate potential energy using integrals in electrostatics
  • Explore advanced topics in electrostatics, such as energy density in electric fields
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Students studying electromagnetism, particularly those tackling problems involving coaxial cylinders and electric fields, as well as educators looking for examples of applying Gauss's Law in practical scenarios.

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Homework Statement



There are 2 long coaxial insulating cylinder. The inner and outer cylinders have radii of a and b and charge densities λ and -λ uniformly distributed on the surface. Calulcate energy per unit length 2 ways (equations below)

Homework Equations



W = \frac{1}{2}\int σ V da
W = \frac{ε0}{2}\int E^2 dτ


The Attempt at a Solution



So using gausses law, with s (radius of cyliunder) < a there is no electric field as there is no enclosed charge. Outside both cylinders there is no E because there is no net charge. SO the only E and energy is between the 2 cylinders.

So I have to do it 2 ways, one with the first and one with the second. I am unsure though how to set up gauss's law to find the E field. Also since we are using line charge how does that change things?

So i wrote |E|* 2*pi*l*s =1/ε0\int λ*2*pi*s*dl

but this doesn't seem right. I am unsure how to deal with the line charge. Do i use like surface charge still but write it as σ = 2*pi*r*dl but what are the limits of integration? I am just a little confused at this part. Help would be nice! Thanks
 
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sorry I wiorked a little bit, is the electric field E = λ/(2*ε0) * (s^2-a^2) where s is the radius on between a and b?

Edit:

I did some looking around and worked a little more and here is where I am at. The electric field in between the two cylinders is \frac{λ}{2*pi*ε0 * s} where s is the radius of the gaussian surface. So then the potential in this area is then

v = -\int E ds and the limits of integration go from b to a (reference at infinity).
so then plugging in E we get

\frac{λ}{2*pi*ε0}* ln(b/a) (negative was used to switch division).

Then do I plug this into the first formula for work? Does σda = λ*l*2*pi*s*ds? What are the limits of integration? From a to b? I think I made a mistake somwehre.
 
Last edited:
Hi guys, so I figured out my main problem with this question. I am having troubles coming to terms with the fact that were using a cylinder but the charge is given in terms of the linear charge density. So when using gauss's law, what is the charge enclosed? Is it just lamba * l?
 

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