History - Evolution of ideas in the field of thermodynamics (statistics in mechanical and gas dynamics)

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Discussion Overview

The discussion revolves around the historical evolution of ideas in thermodynamics, particularly focusing on the contributions of Boltzmann and Maxwell to the concepts of statistics and entropy in mechanical and gas dynamics. Participants explore the attribution of credit for these ideas and the specific contributions that distinguish Boltzmann's work from that of his predecessors.

Discussion Character

  • Historical
  • Debate/contested

Main Points Raised

  • One participant questions why Boltzmann is credited with the notion of statistics related to entropy instead of Maxwell, suggesting that Boltzmann was inspired by Maxwell's earlier work.
  • Another participant argues that while Planck used the idea of entropy in a specific context, Boltzmann provided a more general statistical explanation of the second law of thermodynamics.
  • A participant references the book "Boltzmann's Atom" as a source that discusses these historical questions.
  • One participant asserts that Daniel Bernoulli was the first to conceptualize kinetic theory, which was later expanded by Maxwell, while Boltzmann's key contributions include the derivation of the transport equation and the H-theorem regarding entropy and equilibrium.
  • Another participant emphasizes that Maxwell and Boltzmann achieved similar results in kinetic theory but highlights that Boltzmann's interpretation of entropy as a statistical concept is his most significant contribution.

Areas of Agreement / Disagreement

The discussion features multiple competing views regarding the contributions of Boltzmann and Maxwell, and there is no consensus on the attribution of credit for the development of statistical mechanics and entropy.

Contextual Notes

Participants express uncertainty about the specific contributions of each scientist and the historical context of their work, indicating that the discussion is limited by differing interpretations of their contributions and the evolution of thermodynamic concepts.

Ker_
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Hi,
I have a question regarding the evolution of idea in the field of thermodynamics.
Boltzmann is genereally credited with the notion of stasticis and it's relation to entropy. However, Boltzmann was inspired by the work of Maxwell (who himself followed the conceptual models of Bernoullli for the gas pressure). So why do we credit Boltzmann and not Maxwell for the "paternity" of statistics in mechanical and gas dynamics? What contribution did Boltzmann made that was so determinant?

Also, the equation s=klog(w) that is attributed to boltzmann... wasn't it Max Planck who actually wrote it down when working on his black body problem?

Thanks for helping me!
 
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I think Planck used the idea in a specific situation whereas Boltzmann used the idea in the general situation, providing a statistical explanation of the 2nd Law.
 
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Ker_ said:
Hi,
I have a question regarding the evolution of idea in the field of thermodynamics.
Boltzmann is genereally credited with the notion of stasticis and it's relation to entropy. However, Boltzmann was inspired by the work of Maxwell (who himself followed the conceptual models of Bernoullli for the gas pressure). So why do we credit Boltzmann and not Maxwell for the "paternity" of statistics in mechanical and gas dynamics? What contribution did Boltzmann made that was so determinant?

Also, the equation s=klog(w) that is attributed to boltzmann... wasn't it Max Planck who actually wrote it down when working on his black body problem?

Thanks for helping me!
I'd say the very first having an idea of "kinetic theory" was Daniel Bernoulli, which has been taken up in more generality by Maxwell, as you say. Boltzmann's merit is to have derived the transport equation named after him and the discovery of the "H-theorem" ("Eta theorem"), which in modern formulation says that macroscopic entropy doesn't decrease, and equilibrium has thus to be a state of maximum entropy. The equation for the entropy in the microcanonial ensemble, ##S=-k \ln \Omega##, is indeed due to Max Planck.

The general equation, of course is (for classical statistics),
$$S=-k \int \mathrm{d}^3 x \mathrm{d}^3 p/h^3 f \ln(f/h^3).$$
Of course, Boltzmann couldn't know the quantum-theoretical choice of the "elementary one-particle phase-space cell" of volume ##h^3##, with ##h## Planck's quantum of action.
 
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Ker_ said:
Hi,
I have a question regarding the evolution of idea in the field of thermodynamics.
Boltzmann is genereally credited with the notion of stasticis and it's relation to entropy. However, Boltzmann was inspired by the work of Maxwell (who himself followed the conceptual models of Bernoullli for the gas pressure). So why do we credit Boltzmann and not Maxwell for the "paternity" of statistics in mechanical and gas dynamics? What contribution did Boltzmann made that was so determinant?

Also, the equation s=klog(w) that is attributed to boltzmann... wasn't it Max Planck who actually wrote it down when working on his black body problem?

Thanks for helping me!

"Maxwell and Boltzmann worked on the kinetic theory of gases at about the same time in a slightly different manner and they achieved largely the same results, – all except one! That one result, which escaped Maxwell,
concerned entropy and its statistical or probabilistic interpretation. It provides a deep insight into the strategy of nature and explains irreversibility. That interpretation of entropy is Boltzmann’s greatest achievement, and it places him among the foremost scientists of all times.
"

From the book "A History of Thermodynamics" by Ingo Müller
https://link.springer.com/book/10.1007/978-3-540-46227-9
 
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