Electric Field in a cylindrical Coaxial Capacitor

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SUMMARY

The discussion focuses on calculating the electric field between two infinite coaxial cylindrical tubes with radii a and b, charged with linear charge densities λ and -λ, respectively. Using Gauss' law, the enclosed charge is expressed as q_enc = λL, leading to the equation ∮ E · dA = λL/ε₀. The electric field E can be factored out of the integral due to the symmetry of the cylindrical surface, resulting in E multiplied by the area of the Gaussian surface. The direction of the electric field is confirmed to point from the positively charged tube to the negatively charged tube.

PREREQUISITES
  • Understanding of Gauss' law in electrostatics
  • Familiarity with cylindrical coordinates
  • Knowledge of electric field concepts
  • Basic grasp of charge density and permittivity of free space (ε₀)
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  • Study the application of Gauss' law in different geometries
  • Explore electric field calculations for various charge distributions
  • Learn about the properties of coaxial capacitors
  • Investigate the implications of electric field directionality in electrostatics
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Students of electromagnetism, physics educators, and anyone seeking to deepen their understanding of electric fields in cylindrical geometries.

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Homework Statement



Two infinite coaxial metal cylindrical tubes of radius a and b (a < b) are charged
with charge per unit length (unit [C/m]) \lambda and -\lambda respectively.

Calculate the electric field between the tubes (i.e. for a < r < b)

Where \epsilon_{0} is the permittivity of free space
2. The attempt at a solution

Considering a Gaussian surface with radius R & length L where a < R < b, we can use Gauss' law to find the enclosed charge;

\oint \vec{E}. d\vec{a} = \frac{ q_{enc}}{\epsilon_{0}}

This can then be rewritten as;

\oint \vec{E}. d\vec{a} = \frac{\lambda L}{\epsilon_{0}}

Then I have no clue of where to go. Can take the magnitudes of the vectors and take the E outside or do i have to do something different?
 
Last edited:
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Well you defined a Gaussian surface (a cylinder with radius R). Since it has the same symmetry as the charges, you can claim that the electric field will be constant along your Gaussian surface. That way you can pull it out of the integral, and you will be left with E*A, where A is the area of your Gaussian surface.

The direction of the electric field will point from positive to negative charges.
 
That makes perfect sense thank you very much.
 

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