Flux density inside and outside a coaxial cable.

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SUMMARY

The discussion focuses on calculating the magnetic field (B) inside and outside a coaxial cable using Ampère's Law. For the region outside the coaxial cable, the magnetic field is derived as B = (μI)/(2∏r), where μ is the permeability and I is the current. Inside the coaxial cable, specifically for the region between the inner and outer conductors, the magnetic field is expressed as B = μI(a²)/(πr²b²(2πr - 2πa)). The conversation clarifies the distinction between the regions inside the inner conductor and between the conductors, emphasizing that the area filled with insulator has no current flow.

PREREQUISITES
  • Understanding of Ampère's Law and its application in electromagnetism
  • Familiarity with coaxial cable structure and current flow
  • Knowledge of magnetic permeability (μ) and its significance
  • Basic calculus for evaluating integrals in magnetic field calculations
NEXT STEPS
  • Study the derivation of magnetic fields in different geometries, focusing on coaxial cables
  • Learn about the effects of current density variations in conductors
  • Explore the implications of magnetic fields in insulative materials
  • Investigate the applications of coaxial cables in telecommunications and electrical engineering
USEFUL FOR

Electrical engineers, physics students, and professionals involved in electromagnetic theory and coaxial cable design will benefit from this discussion.

lam58
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For question 4b in the problem sheet attached below, is my working correct for B outside and inside the coaxial cable?




Ans:

Outside coaxial:∫B.dl = μI (the integral is between 0 and 2∏r)
=> B = (μI)/(2∏r)

Inside the coaxial: [tex]\int_{2\pi a}^{2\pi r} B.dI[/tex]
= [tex]μI.\frac{a^2}{\pi r^{2}b^{2}}[/tex]

=> [tex]B[2\pi r - 2\pi a] = μI.\frac{a^2}{\pi r^{2}b^{2}}[/tex]
=>[tex]B = μI.\frac{a^2}{\pi r^{2}b^{2}} * \frac{1}{2\pi r - 2\pi a}[/tex]
 

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It's not obvious what you mean by "outside the coaxial" ... do you mean "between the conductors"?
Notice that the inner current Ia is leftward, but the outer current Ib is rightward.
So, for r>b (outside the outer mesh), how much total I is piercing the Area?

It looks like your "inside the coaxial" is trying to be for r<a, that is, inside the inner conducting wire, assuming uniform current density. This region was not asked for in the problem (perhaps because the current density is not really uniform, in real situations). The region between a and b is filled with insulator, having zero current flow in it (so the right-hand side is constant non-zero).
 
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