Relative permittivity of vacuum aluminum interface?

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SUMMARY

The discussion centers on the relative permittivity of the aluminum-vacuum interface, emphasizing that aluminum, as a conductor, reflects and absorbs electromagnetic (EM) waves. The reflection coefficient is defined by the formula R = 1 - 2 sqrt(2 w e0/sigma), where w is the frequency in radians/sec, e0 is the permittivity of free space, and sigma is the conductivity of aluminum, measured at 37.8e6 S/m. The dielectric function of aluminum can be modeled as ε = ε0 + i(σ/ωε0), highlighting the importance of frequency-dependent conductivity in optical applications, particularly in the context of optical transition radiation (OTR) measurements for charged particle beams.

PREREQUISITES
  • Understanding of electromagnetic wave behavior in conductors
  • Familiarity with the concepts of reflection coefficients and dielectric functions
  • Knowledge of frequency-dependent conductivity in metals
  • Basic principles of optical transition radiation (OTR)
NEXT STEPS
  • Research the derivation and applications of the reflection coefficient formula R = 1 - 2 sqrt(2 w e0/sigma)
  • Study the frequency-dependent conductivity of metals in optical regions
  • Explore the dielectric function of metals as described in Landau and Lifshitz's "Electrodynamics of Continuous Media"
  • Investigate the role of optical transition radiation (OTR) in particle beam profiling
USEFUL FOR

Accelerator physicists, optical engineers, and researchers involved in electromagnetic wave interactions with conductive materials will benefit from this discussion.

omete
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funny but I could not reach the info from net quickly.
 
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Aluminum is a conductor, so the EM wave is attenuated and absorbed. A good conductor reflects the incident wave. the reflection coefficient R is approximately
R = 1 -2 sqrt(2 w e0/sigma)
where w = frequency (radians/sec)
e0 permittivity of free space
sigma = conductivity of metal.
See
https://www.physicsforums.com/showthread.php?t=162915
 
The dielectric constant for a metal is usually hard to find (I don't know if it really is greater than unity) but for most purposes it is irrelevant due to the large conductivity of the metal that will dominate the reflection and transmission properties. Wikipedia gives the conductivity to be 37.8e6 mhos/m (interestingly enough this does not match the given resistivity, oh Wikipedia!). So you can model the permittivity of alumin(i)um simply as:

\epsilon = \epsilon_0+i\frac{\sigma}{\omega\epsilon_0}
where \sigma, the conductivity, is 37.8e6 S/m.
 
thank you very much...
 
holy crap, you guys are awesome
 
Born2bwire,
I don't quite understand your comment that the dielectric constant is irrelevant due to the large conductivity.
In optics one usually choses the polarization P=\int dt j(t) or, in Fourier space, P(\omega)=-j(\omega)/{i \omega}, where j is the induced current in the material (see, e.g. Landau Lifshetz, electrodynamics of continuous media).
Hence the equation you write down is an exact relationship and not just an approximation for any material. However, the conductivity depends generally on frequency and can be complex. In the optical region in metals, it is usually not justified to replace the conductivity by its static value.
The dielectric function of metals is usually inferred from reflectivity measurements and its values in the optical region can be found e.g. in Landolt/Boernstein.
 
OK. It is quite a while then, but I come across this discussion. Then I wanted to add the reason why I need this info, could be of interest to you. It is related to some calculations for OTR (optical transition radiation). You use it to measure the profile of your charged particle beam traveling in vacuum. Yes, I am an accelerator physicist :)
 

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