Entropy

From SklogWiki

Jump to: navigation, search
"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 kB is the Boltzmann constant, m is the index for the microstates, and pm is the probability that microstate m is occupied. In the microcanonical ensemble this gives:

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

where Ω (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:

[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

Personal tools
Namespaces
Variants
Actions
Navigation
Help
Toolbox