Le Chatelier's principle: Difference between revisions

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'''Related reading'''
'''Related reading'''
*[http://dx.doi.org/10.1103/PhysRevE.63.051105  Denis J. Evans, Debra J. Searles, and Emil Mittag "Fluctuation theorem for Hamiltonian Systems: Le Chatelier’s principle", Physical Review E '''63''' 051105 (2001)]
*[http://dx.doi.org/10.1103/PhysRevE.63.051105  Denis J. Evans, Debra J. Searles, and Emil Mittag "Fluctuation theorem for Hamiltonian Systems: Le Chatelier’s principle", Physical Review E '''63''' 051105 (2001)]
*[http://dx.doi.org/10.1063/1.3261849 Pouria Dasmeh, Debra J. Searles, Davood Ajloo, Denis J. Evans, and Stephen R. Williams "On violations of Le Chatelier's principle for a temperature change in small systems observed for short times", Journal of Chemical Physics '''131''' 214503 (2009)]
[[category: classical thermodynamics]]
[[category: classical thermodynamics]]

Latest revision as of 13:31, 3 December 2009

Le Chatelier's principle describes the stability of a system in thermodynamic equilibrium[1][2]:

In response to small deviations away from equilibrium, the system will change in a manner that restores equilibrium.

This translates to conditions on the second derivatives of thermodynamic potentials such as entropy, 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 S(U,\ldots)} . For instance, the entropy is a concave function of its arguments such as internal energy. Thus, one has

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 \frac{\partial^2 S}{\partial U^2} \geq0\ .}

Similarly, specific heats can be shown to be positive definite.

References[edit]

Related reading