EM field due to a long wire submitted to an AC current

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SUMMARY

The discussion focuses on calculating the electromagnetic (EM) fields generated by a long wire carrying an alternating current, specifically I_{0}\sin \omega t. The user seeks to derive the equations for the magnetic field B(t) and electric field E(t) along the X axis, assuming cylindrical symmetry and a uniform current distribution. Key insights include the application of Maxwell's equations and the use of retarded potentials, particularly when the distance to the wire is small compared to the wavelength of the alternating signal.

PREREQUISITES
  • Understanding of Maxwell's equations
  • Knowledge of electromagnetic field theory
  • Familiarity with alternating current (AC) circuits
  • Concept of retarded potentials in electromagnetism
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  • Study the derivation of the electric field E(t) from a long wire using Maxwell's equations
  • Explore the calculation of the magnetic field B(t) around a current-carrying wire
  • Learn about retarded potentials and their applications in electromagnetic theory
  • Investigate the effects of finite wire length on EM field calculations
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Students and professionals in physics, electrical engineering, and anyone interested in electromagnetic theory and applications related to AC currents in long conductors.

jfgobin
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Hello there,

I am having a real stupid moment.

In the space XYZ, a long wire is along the Y axis and is submitted to an alternating current [itex]I_{0}\sin \omega t[/itex]. I am trying to establish the equations for the B(t) and E(t) fields along the X axis.

I assume that the distance to the cable is small in regard to the cable length and that the cable length is small in regard to the wavelength of the alternating signal, so the cable can be seen as having a uniform current along its length. I am pretty sure the problem will have a cylindrical symmetry.

Besides the "use Maxwell's equations", any hint to attack this problem?

Thanks to all!
 
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"use retarded potentials"?

If the distance to the cable is small compared to the wavelength of the alternating signal (if not, the finite cable length is a problem!), you can neglect the time-dependence of the current to get a good approximation.
 

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