Maximal Entrop, Temperature & Energy Transfer

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Discussion Overview

The discussion revolves around the concepts of entropy, temperature, and energy transfer between small systems from a statistical mechanics perspective. Participants explore the implications of entropy maximization in thermal energy transfer, particularly questioning the conventional understanding of energy flow from hot to cold systems.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant suggests that when two systems are brought together, the resulting system will have higher entropy, referencing Kittel's work on statistical properties.
  • Another participant questions the assertion that entropy always increases when systems are combined, citing the Gibbs paradox as a counterexample.
  • A participant expresses uncertainty about the relationship between their original question and the Gibbs paradox, indicating a need for clarification.
  • There is a proposal that for very small systems, it might be conceivable for thermal energy to transfer from a colder system to a hotter system, drawing an analogy to particle collisions.
  • One participant elaborates on the idea of small systems, suggesting that while such energy transfer is statistically possible, it is negligible in a closed system and would increase the thermal gradient.
  • A later reply mentions that microscopic violations of the second law of thermodynamics are allowed by the fluctuation-dissipation theorem and cites experimental evidence supporting this notion.

Areas of Agreement / Disagreement

Participants express differing views on the behavior of entropy in small systems and the implications of the Gibbs paradox. There is no consensus on whether energy can transfer from colder to hotter systems under certain conditions, leaving the discussion unresolved.

Contextual Notes

Limitations include the dependence on the definitions of systems and the assumptions regarding the scale of systems involved. The discussion also touches on unresolved aspects of statistical mechanics and thermodynamics.

azaharak
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Hope you can help my understanding.

Looking at entropy from a stat mech standpoint,
two systems brought together will result in a higher entropy system.

According to Kittel, the most probable configurations will dominate the statisical properties of the combined system, most probable confiigurations are ones that maxmimize the entropy. (pg 36 Thermal Physics Kittel).

For large systems, the multiplicity function or degeneracy is sharply peaked.


The direction of transfer of thermal energy is governed by what situations maximize entropy.

Is it possible to conceive two very small systems (N small), where thermal energy is transferred from the colder system to the hotter system.

I'm thinking that for small systems, it is conceivable that maximal entropy occurs for thermal energy transfering from a cold object to a hot object.

I have also though that this would be the analoge of a two particles colliding, a fast moving one and slow moving one, where the slower particle looses energy in the collision and the faster particle gaining energy.

Thanks

Az
 
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azaharak said:
Hope you can help my understanding.

Looking at entropy from a stat mech standpoint,
two systems brought together will result in a higher entropy system.

Are you sure about that? See, for example, the Gibbs paradox.
 
I'm not sure how that relates to the gibbs paradox



My understanding of the gibbs paradox involves the indistinguishability of particles, a quantum correction.

I can read straight out of Kittel Page 45.

"We can show that the total entropy always increases when two systems are brought into thermal contact."

but this is not answering my original question

Thanks
 
azaharak said:
The direction of transfer of thermal energy is governed by what situations maximize entropy. Is it possible to conceive two very small systems (N small), where thermal energy is transferred from the colder system to the hotter system.

I'm thinking that for small systems, it is conceivable that maximal entropy occurs for thermal energy transfering from a cold object to a hot object.

I have also though that this would be the analoge of a two particles colliding, a fast moving one and slow moving one, where the slower particle looses energy in the collision and the faster particle gaining energy.

A fast particle moving in the y direction, being hit by a slow particle in the x direction, is such a collision. I think it is possible for a small fraction of collisions to transfer heat in such an inverse manner. However, in a closed system, this only increase the thermal gradient, which in turn increases the probability of collisions in the regular sense. The possibility of such a collision is non-zero, but negligible. This is "statistical" mechanics after all.
 
azaharak said:
Is it possible to conceive two very small systems (N small), where thermal energy is transferred from the colder system to the hotter system.

Az

azaharak said:
My understanding of the gibbs paradox involves the indistinguishability of particles, a quantum correction.


but this is not answering my original question

Thanks

Fair enough.

Ok, your question regarding microscopic violations to the second law of thermodynamics, is allowed by the fluctuation-dissipation theorem and has been experimentally demonstrated:

http://prl.aps.org/abstract/PRL/v89/i5/e050601
 

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