Scaling law in thermal phenomena

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dc.creatorKozlowski, M.
dc.creatorMarciak-Kozlowska, J.
dc.date2006-10-29
dc.date.accessioned2026-07-07T07:30:06Z
dc.date.available2026-07-07T07:30:06Z
dc.descriptionIn this paper the scaling law for the relaxation times in thermal phenomena is investigated. It is shown that dependent on the value of the parameter K=E/m(cα)^2,where E is the energy which is delivered to the system, m is the parton mass and α=1/137 for electromagnetic interaction and α=0.16 for strong interaction respectively, heat transport is diffusive, for K<1, or contains the wave component for K>1. For the system with N partons the relaxation time is scaled as τ^N\to N (\hbar/(mcα)^2). Key words: Thermal phenomena, scaling
dc.description7 pages
dc.identifierhttps://arxiv.org/abs/physics/0610267
dc.identifierhttp://arxiv.org/abs/physics/0610267
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/118353
dc.subjectGeneral Physics
dc.titleScaling law in thermal phenomena
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