Radial resistance of coaxial cable

Click For Summary
SUMMARY

The radial resistance of a coaxial cable, where current flows from the inner cylinder to the outer cylinder through silicon, is defined by the formula R = [resistivity * natural log(b/a)] / [2*pi*length]. The derivation involves integrating the differential resistance dR = resistivity*dr/A from the inner radius (a) to the outer radius (b). A critical point of discussion is the dependence of the cross-sectional area on the radial length, which leads to the conclusion that resistance can be simplified to R = resistivity / (2*Pi*L) when considering constant length.

PREREQUISITES
  • Understanding of coaxial cable structure
  • Familiarity with electrical resistance concepts
  • Knowledge of calculus, specifically integration
  • Basic principles of resistivity and its application in materials
NEXT STEPS
  • Study the derivation of resistance in coaxial cables using calculus
  • Learn about the impact of resistivity on electrical components
  • Explore the application of the natural logarithm in physics
  • Investigate the effects of varying lengths and radii on coaxial cable performance
USEFUL FOR

Electrical engineers, physics students, and professionals involved in the design and analysis of coaxial cables and their electrical properties.

azaharak
Messages
152
Reaction score
0
One of the textbooks I've stumbled across states that the radial resistance of a coaxial cable ( current running from inner cylinder to outer cylinder via silicon in between) is given byR = [resistivity * natural log of (b/a)] / [2*pi()*(length of cable)]

where b is the outer radii and a is the inner radiiThe derivation was given as dR= resistivity*dr / A and then integrated from a to b.My question/issue is the dependence of the area on the radial length, I'm not so sure about the correctness of the differential form above.

If you follow through the chain rule with A a function of r

dR/dr= resistivity/Area + (d/dA)*(resistivity*r/Area)*(dA/dr)

which becomes

dR/dr= resistivity/area -[resistivity*r/(Area^2)] * (2*pi()*L)

which becomes

dR/dr=resistivity/area - resistivity/area =0

meaning that the resistance is a constant value which should be

R = resistivity / (2*Pi*L ) where L is the length of the cable (constant)
Help! Thank you very much.Thank you!
 
Last edited:
Physics news on Phys.org
I did not quite follow what you were trying to do; but I never saw you write the area as a function of r, in the first place.

What you need to do is to write what is the cross-sectional area the a radial current 'sees' at a given radiur r...don't call it A, write the formula...it should simply depend on r, pi, and L; then,
integrate the dR from a to b
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 16 ·
Replies
16
Views
3K
  • · Replies 26 ·
Replies
26
Views
4K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 8 ·
Replies
8
Views
2K
Replies
10
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 2 ·
Replies
2
Views
1K
Replies
10
Views
3K
Replies
4
Views
2K