Polarization of Electromagnetic Wave and Faraday's Law of Induction

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SUMMARY

The discussion centers on the application of Faraday's Law of Induction to estimate the induced electromotive force (emf) in a circular wire antenna due to an electromagnetic wave polarized in the x-direction. The wave has a frequency of 1 MHz and an average power density of 1 W/m². The user initially calculated the induced emf but questioned the validity of their approach, particularly regarding the orientation of the magnetic field and the antenna. It was concluded that the induced emf would indeed be zero since the magnetic field component is in the y-direction while the antenna lies in the xy-plane, necessitating a component of the magnetic field along the loop normal for emf induction.

PREREQUISITES
  • Understanding of Faraday's Law of Induction
  • Knowledge of electromagnetic wave polarization
  • Familiarity with Poynting's theorem
  • Basic concepts of complex numbers in electromagnetic theory
NEXT STEPS
  • Study the implications of electromagnetic wave polarization on antenna design
  • Learn about Poynting's theorem and its application in electromagnetic wave analysis
  • Explore the mathematical derivation of Faraday's Law of Induction
  • Investigate the effects of loop orientation on induced emf in different electromagnetic field configurations
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Students and professionals in electrical engineering, particularly those focusing on antenna theory, electromagnetic field analysis, and applications of Faraday's Law in practical scenarios.

sandy.bridge
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Homework Statement


Hey guys. I have an electromagnetic wave traveling in the z direction and polarized in the x direction. The frequency is 1 MHz and average power density is 1 W/m^2. An antenna in the shape of a circular wire is in the xy-plane centred at the origin. I would like to use Faraday's Law of Induction to estimate the amplitude of the emf induced on antenna from the wave passing through it. Assume the radius is 1cm, and that the wavelength of the electromagnetic wave is much larger than this.

The Attempt at a Solution


Since it is polarized in the x-direction I can assume \vec{E}=E_oe^{j(ωt-kz)}\vec{x}.

Therefore, \vec{H}=\frac{\vec{∇}×\vec{E}}{-jμ_oω}=\frac{E_o}{120π}e^{j(ωt-kz)}\vec{y}

Since <\vec{S}>=0.5Re[\vec{E}×\vec{H^*}]=1W/m^2\vec{z}, I get E_o=\sqrt{2}

From here I get that the induced emf is -μ_o \int_S ∂\vec{H}/∂t . d\vec{S}

which I crunched to be \frac{-μ_o \sqrt{2}jω(0.0001π)e^{j(ωt-kz)}}{120π}

I have never encountered this when the magnetic field has complex components. Would I merely take the real component (hence the sine term), or have I messed up somewhere?
 
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I found some errors in this. Eo should have came out to sqrt(240pi) and the magnetic wave should have been sqrt(240pi)/(120pi)e^(j(wt-kz)) in the y direction.

My question is this:
since the magnetic field component of the electromagnetic wave is in the y direction and the ring of wire is situated in the xy plane, would the induced emf not be zero?
 
sandy.bridge said:
I found some errors in this. Eo should have came out to sqrt(240pi) and the magnetic wave should have been sqrt(240pi)/(120pi)e^(j(wt-kz)) in the y direction.

My question is this:
since the magnetic field component of the electromagnetic wave is in the y direction and the ring of wire is situated in the xy plane, would the induced emf not be zero?

Yes. The H field needs to point in the direction of the loop normal or at least have a component along the normal. Since H has only a y component, the loop normal should also point along the y direction. So it can't be in the x-y plane since then the loop normal is along z.

Otherwise your approach is OK. Use Poynting to compute H. There should be no complex numbers involved. Then use faraday' s induction law.
 

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