Speed of light in a superconductor

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SUMMARY

The discussion centers on the behavior of light in superconductors, specifically addressing the equation for the speed of light in a material, given by c = √(1/(εμ)). It highlights that in superconductors, the magnetic susceptibility (χ_m) is -1, leading to a relative permeability (μ_r) of 0, which suggests an infinite speed of light (c = ∞). This conclusion is challenged by the understanding that superconductors act as perfect diamagnets, preventing electromagnetic radiation from penetrating, thus demonstrating that light does not propagate within an ideal superconductor.

PREREQUISITES
  • Understanding of electromagnetic theory, specifically Maxwell's equations
  • Familiarity with the concepts of permittivity (ε) and permeability (μ)
  • Knowledge of superconductivity and its properties, including perfect diamagnetism
  • Basic grasp of phase velocity versus group velocity in wave propagation
NEXT STEPS
  • Research the implications of negative index of refraction materials on light propagation
  • Study the relationship between resistivity and penetration depth in superconductors
  • Explore the concept of phase velocity in electromagnetic waves and its relevance to superconductors
  • Investigate the conditions under which light can exceed the speed of light in a vacuum, particularly in anomalous dispersion scenarios
USEFUL FOR

Physicists, electrical engineers, and materials scientists interested in the properties of superconductors and their effects on electromagnetic wave propagation.

Domenicaccio
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Could you please spot where is the fault in this reasoning? I suspect that some of the relations may not be applicable and needs to be substituted with something else (or I'm just making a gross mistake as usual...):

Speed of light in a material:

c=\sqrt{\frac{1}{\epsilon\mu}}

where permettivity is

\mu=\mu_r\mu_0

and suscettivity is

\chi_m=\mu_r - 1

which describes the magnetization of the material due to an external magnetic field

M=\chi_m H

-------------------------

A superconductor behaves like a perfectly diamagnetic material, suppressing the internal field B because

\chi_m = - 1

M=-H

therefore

\mu_r = 0

\mu = 0

c=infinite

which clearly makes no sense...
 
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there are also negative index of refraction materials
which also mess that up.

i think the subtlety is the phase vs group velocity
of the light waves.http://en.wikipedia.org/wiki/Phase_velocity

"...The phase velocity of electromagnetic radiation may under certain circumstances (e.g. in the case of anomalous dispersion) exceed the speed of light in a vacuum, but this does not indicate any superluminal information or energy transfer..."
 
Last edited:
Also, in a perfect conductor, \epsilon = \infty. I don't know if this applies to superconductors (but they do offer practically zero resistance, yes?).
 
IIRC, the penetration depth of light into a conductor is proportionate to the resistivity, so in a perfect conductor light won't penetrate at all (the charge carries at the surface absorb all the light that isn't reflected).
 
What you are discovering is that you don't have electromagnetic radiation inside an ideal superconductor.
 

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