Entropy: Difference between revisions

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The '''entropy''', S, is defined by
The '''entropy''', S, is defined by
:<math>\left. S \right. = -k_B \sum_m p_m \ln p_m</math>
where <math>k_B</math> is the [[Boltzmann constant]], ''m'' is the index for the microstates, and <math>p_m</math>
is the probability that microstate ''m'' is occupied.
In the [[microcanonical ensemble]] this gives:


:<math>\left.S\right. = k_B \ln \Omega</math>
:<math>\left.S\right. = k_B \ln \Omega</math>


where <math>k_B</math> is the [[Boltzmann constant]] and <math>\Omega</math> (sometimes written as <math>W</math>)
where <math>\Omega</math> (sometimes written as <math>W</math>)
is the number of microscopic configurations that result in the observed macroscopic description of the thermodynamic system.
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 | classical thermodynamics]] and  
This equation provides a link between [[Classical thermodynamics | classical thermodynamics]] and  
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*[http://dx.doi.org/10.1119/1.1971557 E. T. Jaynes "Gibbs vs Boltzmann Entropies",  American Journal of Physics '''33''' pp. 391-398 (1965)]
*[http://dx.doi.org/10.1119/1.1971557 E. T. Jaynes "Gibbs vs Boltzmann Entropies",  American Journal of Physics '''33''' pp. 391-398 (1965)]
*[http://www.ucl.ac.uk/~ucesjph/reality/entropy/text.html S. F. Gull "Some Misconceptions about Entropy" in Brian Buck and Vincent A. MacAulay (Eds.) "Maximum Entropy in Action", Oxford Science Publications (1991)]
*[http://www.ucl.ac.uk/~ucesjph/reality/entropy/text.html S. F. Gull "Some Misconceptions about Entropy" in Brian Buck and Vincent A. MacAulay (Eds.) "Maximum Entropy in Action", Oxford Science Publications (1991)]
*[http://dx.doi.org/10.1119/1.1287353 Daniel F. Styer "Insight into entropy",  American Journal of Physics '''68''' pp. 090-1096 (2000)]
*[http://dx.doi.org/10.1119/1.1990592 Karl K. Darrow "The Concept of Entropy",  American Journal of Physics '''12''' pp.  183-196 (1944)]
 
*[http://dx.doi.org/10.1119/1.1287353 Daniel F. Styer "Insight into entropy",  American Journal of Physics '''86''' pp. 1090-1096 (2000)]
==References==
==References==
#[http://dx.doi.org/10.1063/1.1670348 William G. Hoover "Entropy for Small Classical Crystals", Journal of Chemical Physics '''49''' pp. 1981-1982 (1968)]   
#[http://dx.doi.org/10.1063/1.1670348 William G. Hoover "Entropy for Small Classical Crystals", Journal of Chemical Physics '''49''' pp. 1981-1982 (1968)]   
[[category:statistical mechanics]]
[[category:statistical mechanics]]

Revision as of 11:25, 29 August 2007

The entropy, S, is defined by

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left. S \right. = -k_B \sum_m p_m \ln p_m}

where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle k_B} is the Boltzmann constant, m is the index for the microstates, and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle p_m} is the probability that microstate m is occupied. In the microcanonical ensemble this gives:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left.S\right. = k_B \ln \Omega}

where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \Omega} (sometimes written as Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 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

Arrow of time

See also:

Interesting reading

References

  1. William G. Hoover "Entropy for Small Classical Crystals", Journal of Chemical Physics 49 pp. 1981-1982 (1968)