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Chapter 6
Chapter 6

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Document

... A gas can be ionized under non equilibrium conditions (too low temperature for equilibrium ionization) with constant energy dissipation, like in electric discharges, photoionized media, preshock regions, and so on. ...
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Thermodynamic functions - Phase Transformations Group

Course Home - Haldia Institute of Technology
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... These are energetically equivalent states for the expansion of a gas. It doesn’t matter, in terms of potential energy, whether the molecules are all in one flask, or evenly distributed. But one of these states is more probable than the other two. © 2014 Pearson Education, Inc. ...
Chapter 6 Thermodynamics and the Equations of Motion
Chapter 6 Thermodynamics and the Equations of Motion

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Chapter 12 - HCC Learning Web

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Bioengineering Thermodynamics - PORTO

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A More Efficient Way to Describe Interacting Quantum Particles in 1D

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H-theorem



In classical statistical mechanics, the H-theorem, introduced by Ludwig Boltzmann in 1872, describes the tendency to increase in the quantity H (defined below) in a nearly-ideal gas of molecules. As this quantity H was meant to represent the entropy of thermodynamics, the H-theorem was an early demonstration of the power of statistical mechanics as it claimed to derive the second law of thermodynamics—a statement about fundamentally irreversible processes—from reversible microscopic mechanics.The H-theorem is a natural consequence of the kinetic equation derived by Boltzmann that has come to be known as Boltzmann's equation. The H-theorem has led to considerable discussion about its actual implications, with major themes being: What is entropy? In what sense does Boltzmann's quantity H correspond to the thermodynamic entropy? Are the assumptions (such as the Stosszahlansatz described below) behind Boltzmann's equation too strong? When are these assumptions violated?↑
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