Does a randomly polarized beam have higher entropy than a fully polarized beam?

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Discussion Overview

The discussion revolves around the entropy of polarized versus unpolarized light, specifically whether a randomly polarized beam has higher entropy than a fully polarized beam. Participants explore theoretical implications, definitions of entropy, and the relationship between polarization and entropy in the context of thermodynamics.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants propose that unpolarized light has higher entropy due to the greater number of possible orientations compared to polarized light.
  • Others express confusion about the application of entropy definitions, particularly in relation to thermodynamic principles.
  • A participant suggests that splitting an unpolarized beam into polarized components could violate the second law of thermodynamics, raising questions about energy conservation and entropy changes.
  • Another viewpoint indicates that polarized light may not be as bright, and that converting part of the light into heat could potentially increase overall entropy.
  • Some participants discuss the independence of polarization states and the challenges in recombining polarized beams, questioning how these factors relate to entropy.
  • A later reply mentions that monochromatic radiation does not have an associated thermodynamic temperature, yet argues that a randomly polarized beam likely has higher entropy due to its statistical nature.

Areas of Agreement / Disagreement

Participants express differing opinions on whether unpolarized or polarized light has higher entropy, with no consensus reached. The discussion remains unresolved, with multiple competing views presented.

Contextual Notes

Participants highlight limitations in their understanding of thermodynamics and entropy definitions, indicating a reliance on specific contexts and assumptions that may not be universally applicable.

Phrak
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Which has lower entropy, a beam of unpolarized light, or this same beam split into polarized components?
 
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The more possibilities, for example the more possibilities for the orientation of something, the higher the entropy.
 
Phrak said:
Which has lower entropy, a beam of unpolarized light, or this same beam split into polarized components?

Wow! I've only been introduced the change of entropy as being [tex]\Delta S = \int \frac{dQ}{T}[/tex] which obviously cannot be applied here.
I'd love to learn any other definition of it.
My intuition tells me that the unpolarized light is the one with higher entropy, as suggested by ericgrau.
 
Thermodynamics was my worst subject. I don't know how I managed to pass, so I'm very baffled.

If one can split an unpolarized beam into two polarized beams without significant loses, it would seem to violate the second law of thermodynamics in some way. Can someone help me overcome my ignorance?
 
Polarized light isn't as bright, that may be it. If anything changing part of the light into heat and reducing the amount of light energy (which is relatively low entropy) may increase overall entropy.
 
Last edited:
Neither.

Say you arrange that one polarisation is reflected, the other transmitted, by some optic. Now, if both beams are totally reflected back, won't they perfectly recombine? Aren't the polarisations independent degrees of freedom right from the beginning?
 
cesiumfrog said:
Neither.

Say you arrange that one polarisation is reflected, the other transmitted, by some optic. Now, if both beams are totally reflected back, won't they perfectly recombine? Aren't the polarisations independent degrees of freedom right from the beginning?

Well... I did say it was my worst subject. How are they independent?
 
Recall that monochromatic radiation (of any poalrization state) does not have a thermodynamic temperature associated with it- only blackbody radiation does.

Even so, it seems logical to think a randomly polarized beam has a higher entropy than a fully polarized beam because polarization is a statistical measure of the beam properties. Splitting the randomly polarized beam into two orthogonal components is not the problem, but recombining them is- it is surprisingly tricky to generate a randomly polarized beam (usually moving ground glass surfaces or other scattering processes are involved).
 

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