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The Gibbs paradox

Abstract:
The Gibbs Paradox is essentially a set of open questions as to how sameness of gases or fluids (or masses, more generally) are to be treated in thermodynamics and statistical mechanics. They have a variety of answers, some restricted to quantum theory (there is no classical solution), some to classical theory (the quantum case is different). The solution offered here applies to both in equal measure, and is based on the concept of particle indistinguishability (in the classical case, Gibbs’ notion of ‘generic phase’). Correctly understood, it is the elimination of sequence position as a labelling device, where sequences enter at the level of the tensor (or Cartesian) product of one-particle state spaces. In both cases it amounts to passing to the quotient space under permutations. ‘Distinguishability’, in the sense in which it is usually used in classical statistical mechanics, is a mathematically convenient, but physically muddled, fiction.
Publication status:
Published
Peer review status:
Peer reviewed

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Files:
Publisher copy:
10.3390/e20080552

Authors


More by this author
Institution:
University of Oxford
Division:
HUMS
Department:
Philosophy Faculty
Oxford college:
Merton College
Role:
Author
ORCID:
0000-0002-8292-3014


Publisher:
MDPI
Journal:
Entropy More from this journal
Volume:
20
Issue:
8
Pages:
552
Publication date:
2018-07-25
Acceptance date:
2018-07-24
DOI:
EISSN:
1099-4300


Language:
English
Keywords:
Pubs id:
pubs:917734
UUID:
uuid:82a6f3e5-4769-4b78-ad4d-ac962ae9c46e
Local pid:
pubs:917734
Source identifiers:
917734
Deposit date:
2019-02-05

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