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Entropy and sign conventions

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Abstract

It is a fundamental cornerstone of thermodynamics that entropy (\(S_{U,V}\)) increases in spontaneous processes in isolated systems (often called closed or thermally closed systems when the transfer of energy as work is considered to be negligible) and achieves a maximum when the system reaches equilibrium. But with a different sign convention entropy could just as well be said to decrease to a minimum in spontaneous constant UV processes. It would then change in the same direction as the thermodynamic potentials in spontaneous processes. This article discusses but does not advocate such a change.

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Notes

  1. Adopted for example by Lewis and Randell (1923), Prigogine and Defay (1954), Moore (1962), ?.

  2. Adopted for example by Jones and Dugan (1996), Denbigh (1966), Klotz (1964), Reiss (1965).

  3. It is often said that entropy increases in every irreversible process if the environment of the system is included as part of the system, though when the environment is the rest of the universe, as it often is, this is questionable. Cosmologists are still debating the entropy of the universe (Carroll 2010).

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Acknowledgements

I thank Norm Evensen for many useful discussions on this and other thermodynamic topics, Karyn and Brendan Bradley Gorra for help with the figures, and Grant Garven for encouraging me to persist after several journal rejections with no peer review.

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Correspondence to G. M. Anderson.

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Anderson, G.M. Entropy and sign conventions. Found Chem 25, 119–125 (2023). https://doi.org/10.1007/s10698-022-09463-6

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