Quasi-static Approximation for coaxial wires

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SUMMARY

The discussion centers on the dominant field in a coaxial cable setup with inner radius 'a' and outer radius 'b', where voltage sources are uniformly distributed along the z-axis and a short circuit exists at z=0. The dominant field under DC conditions is identified as the electric field, contrary to the initial assumption that the magnetic field would prevail due to the presence of current. The scenario is complicated by the perfect conductivity of the cable and the implications of infinite current in a steady state, leading to the conclusion that the electric field is indeed the dominant factor when considering the application of voltage as a step function.

PREREQUISITES
  • Understanding of coaxial cable geometry and parameters (inner radius 'a', outer radius 'b', length 'L')
  • Knowledge of DC circuit theory and the behavior of electric and magnetic fields
  • Familiarity with the concept of characteristic impedance in transmission lines
  • Basic principles of electromagnetic theory, particularly in relation to perfect conductors
NEXT STEPS
  • Study the effects of voltage sources in coaxial cables under DC conditions
  • Learn about the concept of characteristic impedance and its role in transmission line theory
  • Explore the implications of perfect conductivity in electrical circuits
  • Investigate the differences between electric and magnetic fields in steady-state conditions
USEFUL FOR

Electrical engineers, physics students, and anyone involved in the analysis of coaxial cables and electromagnetic fields in DC circuits.

StasKO
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Homework Statement



A coaxial cable with inner radius a and outer radius b lies on the z-axis (such that the cable's axis merges with the z-axis). its length (along z-axis) is L. at z=-L there are voltage sources that are distributed uniformly connecting the inner wire to the outer one. at z=0 there is a short circuit. all conductors are perfect.

what is the dominant field?

Homework Equations



the dominant field is the one that exists in DC conditions

The Attempt at a Solution



Im totally stuck. in a previos question instead of the voltage sources there were current sources so that was easy - at DC only current flows so the magnetic field is the dominant. I think that since there is a short circuit and all conductors are perfect than changing the source does not change anything since current still flows in DC and the magnetic field is the dominant but in the solution it says that its the electric field that is dominant.

thanks!
 
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"voltage sources at z = -L"? How can you have more gthan one source at one point?

Anyway, the situation is impossible in the steady state since the cable, being a perfect conducror and shorted at the z=0 end, would result in infinite current.

However, if you assume the voltage is appplied as a step at t=0 and L is long enough, then the current is limited to the characteristic impedance of the cable until the return voltage hits the source, or T = 2L/v with v the velocity of propagation.

Ayway, I think the question of what is "dominant" is extremely imprecise.
 

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