Light hitting a dielectric, increase of momentum

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SUMMARY

Light propagating through a dielectric medium, such as one with a refractive index of n=1.33, experiences an increase in momentum compared to its momentum in a vacuum (n=1). This extra momentum is transferred to the dielectric medium, although it is momentary, as the light recovers this momentum upon exiting the dielectric. The discussion highlights the importance of the Poynting vector in understanding momentum transfer in electromagnetic fields, particularly in contrast to lossy media where energy is absorbed and transferred to the medium.

PREREQUISITES
  • Understanding of wavevector and refractive index in optics
  • Familiarity with the Poynting vector and its significance in electromagnetic theory
  • Knowledge of momentum conservation principles in physics
  • Basic concepts of dielectric materials and their properties
NEXT STEPS
  • Research the implications of radiation pressure in dielectric materials
  • Study the Poynting vector and its applications in electromagnetic field analysis
  • Explore the behavior of light in lossy media and the effects of complex dielectric functions
  • Investigate the relationship between light frequency and plasma frequency in various materials
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Physicists, optical engineers, and anyone interested in the interaction of light with dielectric materials and the principles of momentum transfer in electromagnetic fields.

Repetit
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When light propagates in a dielectric its wavevector is given by:

<br /> k = \frac{\omega n}{c}<br />

where n is the refractive index. If light propagates in vacuum n=1 the momentum is \omega / c but if light propagates in a dielectric of for example n=1.33 the momentum is increased beyond the value of the momentum in vacuum? Where does this extra momentum come from? It has to come from the dielectric somehow but how does this work?
 
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There is a momentum transfer to the medium. The momentum transfer is momentary since the light will recover that momentum (neglecting reflections) upon exiting the dielectric.

Do a google on radiation pressure and linear photon momentum conservation and you will probably get some papers that go into the sordid details.

Claude.
 
Repetit said:
When light propagates in a dielectric its wavevector is given by:

<br /> k = \frac{\omega n}{c}<br />

where n is the refractive index. If light propagates in vacuum n=1 the momentum is \omega / c but if light propagates in a dielectric of for example n=1.33 the momentum is increased beyond the value of the momentum in vacuum?

...but if the light propagates at a frequency that is much greater than the plasma frequency of the medium then 'n' is less than one... and if the light has a frequency that is exactly equal to the plasma frequency then n=0!

Anyways, the problem is that you can't really say that the light "has more momentum" in the medium since the momentum is not a local quantity for a field--we are not talking about photons here, we are talking about photons en masse as macroscopic electric fields--In this case, we have the poynting vector to tell us about the momentum of the field, but the pointing vector is not really a "local" quantity in the sense that it must be intergated over closed surfaces to obtain sensable results... You could integrate the poynting vector over the front and back faces of the dielectric slab to see that no energy is transferred to it.

This is to be contrasted with a "lossy" medium (with a complex dielectric function) where there will be energy transferred to the "slab" (which heats it up).

Cheers.
 

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