Frustrated total internal reflection: Where does energy come from?

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SUMMARY

This discussion centers on the phenomenon of frustrated total internal reflection (FTIR) and its implications for energy transfer between optical media. When light undergoes total internal reflection at the boundary of an optically dense medium to a thinner medium, the Poynting vector perpendicular to the boundary is zero, indicating no energy flow. However, introducing a second optically denser medium allows energy to propagate through the evanescent field, despite the initial zero Poynting vector in the thin medium. The Goos-Hanchen effect is also relevant in understanding this energy transfer.

PREREQUISITES
  • Understanding of Poynting vector in electromagnetism
  • Knowledge of optical density and refractive index concepts
  • Familiarity with total internal reflection principles
  • Basic grasp of evanescent waves and their properties
NEXT STEPS
  • Research the Goos-Hanchen effect in detail
  • Study the mathematical formulation of evanescent fields
  • Explore applications of frustrated total internal reflection in optical devices
  • Investigate the implications of FTIR in fiber optics technology
USEFUL FOR

Physicists, optical engineers, and students studying wave optics who are interested in the principles of light propagation and energy transfer in different media.

greypilgrim
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Hi,

When we have total internal reflection of light at the boundary of an optically dense to an optically thinner medium, one can show that the component of the Poynting vector perpendicular to the boundary is zero, i.e. there is no energy flow into the thinner medium. However, the electrical field is not zero in the thinner medium but decays exponentially with a certain penetration depth.

If we now add an optically denser medium just behind the thin medium, we get frustrated total internal reflection, i.e. a propagating wave in the second dense medium with a nonzero Poynting vector. How is it possible that energy crosses the thin medium although the Poynting vector in the thin medium is zero?
 
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The evanescent field is "stationary" in the first case - hence no energy is flowing out and the Poynting vector is zero.

With the second piece of material brought close to the evanescent field it will penetrate (no longer frustrated because now it is low to high index), so it leaks through. Once it leads through into the second piece of glass the field can propagate.

You should also look into the Goos-Hanchen effect: http://en.wikipedia.org/wiki/Goos–Hänchen_effect

The following article goes into more depth:
http://www.cleyet.org/Misc._Physics/Microwave-Optics/Evanescent-FTIR/FTIR review.pdf
 

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