Entropy

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"Energy has to do with possibilities. Entropy has to do with the probabilities of those possibilities happening. It takes energy and performs a further epistemological step."
Constantino Tsallis [1]

Entropy was first described by Rudolf Julius Emanuel Clausius in 1865 [2]. The statistical mechanical desciption is due to Ludwig Eduard Boltzmann (Ref. ?).

Contents

[edit] Classical thermodynamics

In classical thermodynamics one has the entropy, \(S\), \[{\mathrm d} S = \frac{\delta Q_{\mathrm {reversible}}} {T} \]

where \(Q\) is the heat and \(T\) is the temperature.

[edit] Statistical mechanics

In statistical mechanics entropy is defined by

\[\left. S \right. = -k_B \sum_m p_m \ln p_m\]

where \(k_B\) is the Boltzmann constant, m is the index for the microstates, and \(p_m\) is the probability that microstate m is occupied. In the microcanonical ensemble this gives:

\[\left.S\right. = k_B \ln \Omega\]

where \(\Omega\) (sometimes written as \(W\)) is the number of microscopic configurations that result in the observed macroscopic description of the thermodynamic system. This equation provides a link between classical thermodynamics and statistical mechanics

[edit] Arrow of time

Articles:

Books:

  • Steven F. Savitt (Ed.) "Time's Arrows Today: Recent Physical and Philosophical Work on the Direction of Time", Cambridge University Press (1997) ISBN 0521599458
  • Michael C. Mackey "Time's Arrow: The Origins of Thermodynamic Behavior" (1992) ISBN 0486432432
  • Huw Price "Time's Arrow and Archimedes' Point New Directions for the Physics of Time" Oxford University Press (1997) ISBN 978-0-19-511798-1

[edit] See also:

[edit] References

  1. http://www.mlahanas.de/Greeks/new/Tsallis.htm
  2. R. Clausius "Ueber verschiedene für die Anwendung bequeme Formen der Hauptgleichungen der mechanischen Wärmetheorie", Annalen der Physik und Chemie 125 pp. 353-400 (1865)

Related reading

[edit] External links

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