Light hitting a dielectric, increase of momentum

In summary, when light propagates in a dielectric its wavevector is increased beyond the value of the momentum in vacuum due to a momentum transfer from the dielectric.
  • #1
Repetit
128
2
When light propagates in a dielectric its wavevector is given by:

[tex]
k = \frac{\omega n}{c}
[/tex]

where n is the refractive index. If light propagates in vacuum n=1 the momentum is [tex]\omega / c[/tex] 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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  • #2
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.
 
  • #3
Repetit said:
When light propagates in a dielectric its wavevector is given by:

[tex]
k = \frac{\omega n}{c}
[/tex]

where n is the refractive index. If light propagates in vacuum n=1 the momentum is [tex]\omega / c[/tex] 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.
 

FAQ: Light hitting a dielectric, increase of momentum

How does light hitting a dielectric affect its momentum?

When light hits a dielectric material, it transfers some of its momentum to the material. This is due to the interaction between the electric field of the light and the charged particles in the material, causing them to be displaced and creating a net momentum in the direction of the light's propagation.

Does light always transfer momentum when it hits a dielectric?

No, the amount of momentum transferred depends on the properties of the dielectric material. Materials with higher refractive indices will generally experience a larger transfer of momentum from light, while materials with lower refractive indices may experience little to no transfer.

How does the angle of incidence affect the momentum transfer of light hitting a dielectric?

The angle of incidence does not have a significant effect on the total momentum transferred, but it can affect the direction of the momentum. When light hits a dielectric at an angle, the momentum transfer is split between a component parallel to the surface and a component perpendicular to the surface.

Can the momentum transfer of light hitting a dielectric be reversed?

Yes, the momentum transfer can be reversed if the light is reflected off the dielectric surface. In this case, the net momentum change for the light-dielectric system is zero, but the momentum transfer is still present in the form of a change in the direction of the reflected light.

What is the practical application of studying the momentum transfer of light hitting a dielectric?

Understanding the momentum transfer of light and its interaction with dielectric materials is important in various fields such as optics, photonics, and materials science. It allows us to develop technologies such as lenses, optical fibers, and solar cells, and also plays a role in understanding the behavior of light in complex systems.

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