On the classical energy equipartition theorem

Please use this identifier to cite or link to this item: http://dspace.mediu.edu.my:8181/xmlui/handle/123456789/2894

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DC Field	Value	Language
dc.creator	Lima J. A. S.	-
dc.creator	Plastino A. R.	-
dc.date	2000	-
dc.date.accessioned	2013-05-29T23:51:33Z	-
dc.date.available	2013-05-29T23:51:33Z	-
dc.date.issued	2013-05-30	-
dc.identifier	http://www.scielo.br/scielo.php?script=sci_arttext&pid=S0103-97332000000100019	-
dc.identifier	http://www.doaj.org/doaj?func=openurl&genre=article&issn=01039733&date=2000&volume=30&issue=1&spage=176	-
dc.identifier.uri	http://koha.mediu.edu.my:8181/jspui/handle/123456789/2894	-
dc.description	A general proof of the energy equipartition theorem is given. Our derivation holds for any distribution function depending on the phase space variables only through the Hamiltonian of the system. This approach generalizes the standard theorem in two main directions. On the one hand, it considers the contribution to the total mean energy of homogeneous functions having a more general type than the ones usually discussed in the literature. On the other hand, our proof does not rely on the assumption of a Boltzmann-Gibbs exponential distribution.	-
dc.publisher	Sociedade Brasileira de Física	-
dc.source	Brazilian Journal of Physics	-
dc.title	On the classical energy equipartition theorem	-
Appears in Collections:	Physics and Astronomy

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