David Bourget (Western Ontario)
David Chalmers (ANU, NYU)
Rafael De Clercq
Jack Alan Reynolds
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Synthese 81 (3):283 - 312 (1989)
It is only when mixing two or more pure substances along a reversible path that the entropy of the mixing can be made physically manifest. It is not, in this case, a mere mathematical artifact. This mixing requires a process of successive stages. In any finite number of stages, the external manifestation of the entropy change, as a definite and measurable quantity of heat, isa fully continuous function of the relevant variables. It is only at an infinite and unattainable limit thata non-uniform convergence occurs. And this occurs when considered in terms of the number of stages together with a distinguishability parameter appropriate to the particular device which is used to achieve reversibility. These considerations, which are of technological interest to chemical engineers, resolve a paradox derived in chemical theory called Gibbs'' Paradox.
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References found in this work BETA
Michael J. Zenzen (1985). Entropy in Relation to Incomplete Knowledge. Monograph Collection (Matt - Pseudo).
Citations of this work BETA
Peter M. Ainsworth (2012). The Gibbs Paradox and the Definition of Entropy in Statistical Mechanics. Philosophy of Science 79 (4):542-560.
Robin Findlay Hendry (2010). Entropy and Chemical Substance. Philosophy of Science 77 (5):921-932.
D. Costantini & U. Garibaldi (1997). A Probabilistic Foundation of Elementary Particle Statistics. Part I. Studies in History and Philosophy of Science Part B 28 (4):483-506.
V. Mosini (1995). Fundamentalism, Antifundamentalism, and Gibbs' Paradox. Studies in History and Philosophy of Science Part B 26 (2):151-162.
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