What is the equation for capacitance of a coaxial cable?

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Homework Help Overview

The original poster seeks a general equation for the capacitance of a coaxial cable per meter length, providing a diagram and details about the radii and dielectric material. The outer conductor is grounded, with a voltage of 0V.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Some participants suggest using Gauss's law and setting an arbitrary charge for analysis. Others discuss the integration of electric field expressions to find the potential difference, questioning the application of certain equations and the need for integration.

Discussion Status

The discussion is ongoing, with participants exploring different approaches to derive the capacitance equation. Some guidance has been offered regarding the use of Gauss's law and the integration of electric field expressions, but no consensus has been reached on the solution.

Contextual Notes

Participants note the challenge of applying equations meant for parallel plate capacitors to the coaxial configuration and the necessity of integrating to find the potential difference across the conductors.

jumpboy
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Homework Statement



http://smg.photobucket.com/albums/v68/jumpboyb/?action=view&current=scan0001.jpg"
Pretty much looking for a general equation for capacitance of a coaxial cable per meter length.

given:
-a diagram (click link)
-two radii
-dielectric material
-outer conductor is grounded (V = 0V)

Homework Equations


C = Q/V
C=A/d\epsilon0


The Attempt at a Solution


used the second equation but won't work since its for a parallel plate capacitor.

thats it! I'm lost on this one
 
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I think the best way to approach this problem is with Gauss's law. You need to set an arbitrary charge (it will vanish in the end.). Use a cylinder as your Gaussian surface. Hope this helps
 
Still stuck. Here's what I did with Gauss' Law in mind. (btw, the answer is (2pi\epsilon)/ln(R2/R1) and that's not pi to the epsilon not power btw.)

So, with Gauss, you have integral of E dot dA which equals Q/\epsilon.

Capacitance - Q=VC...so subsitute that back into the gauss equation so you have...

EA = VC/epsilon \Rightarrow C= EA[epsilon]/V

Electric potential is the negative rate of change of a electric field...ie E = -dV/ds = -V/r where r = R2 - R1

C=-rA[epsilon]=-2pi(r)3[epsilon]

and yea...nothing. I see I need to integrate something, but idk where or what logic to use for it.
 
To get V you must integrate the expression for E with respect to dr. You can't just use E = -V/r which is true only for the simplest 1D case.
 
Right, try adding the integral of E dot dl or dr (whatever you guys call it.) into your arsenal.
 
the expression you want to integrate is dV = -[Q/(2Pi*R)] with limits from R1 to R2 (inner to outter). This is obtained through gauss's law, saying that EA = Qin/Episilon, solving for E and substituting for the original integral of dV = -[E dot ds]. The area "A" is 2*Pi*r because after the length is taken into acount, it will account for the surface area.
 

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