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dc.contributor.authorAkyildiz, FT
dc.contributor.authorBellout, H
dc.date.accessioned2020-06-21T15:37:07Z
dc.date.available2020-06-21T15:37:07Z
dc.date.issued2005
dc.identifier.issn0096-3003
dc.identifier.urihttps://doi.org/10.1016/j.amc.2004.01.020
dc.identifier.urihttps://hdl.handle.net/20.500.12712/21155
dc.descriptionWOS: 000226860100009en_US
dc.description.abstractThe onset of chaotic motion in Newtonian fluid with a temperature dependent viscosity is explored in the context of the Rayleigh-Benard thermal convection setup. Galerkin truncation is used to derive a low-order dynamical system (generalized Lorenz system) from the governing equations which reduces to the classical Lorenz system for a Newtonian fluid with a constant viscosity. The effect of the temperature dependent viscosity on the nonlinear solutions is analyzed by considering projections in the phase-space. Also, time signature of the solutions is investigated. The onset of chaotic motion is also discussed in detail for different values of temperature dependent viscosity in this paper. (C) 2004 Published by Elsevier Inc.en_US
dc.language.isoengen_US
dc.publisherElsevier Science Incen_US
dc.relation.isversionof10.1016/j.amc.2004.01.020en_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjecttemperature dependent viscosityen_US
dc.subjectgeneralized Lorenz modelen_US
dc.subjectchaosen_US
dc.titleChaos in the thermal convection of a Newtonian fluid with a temperature dependent viscosityen_US
dc.typearticleen_US
dc.contributor.departmentOMÜen_US
dc.identifier.volume162en_US
dc.identifier.issue3en_US
dc.identifier.startpage1103en_US
dc.identifier.endpage1118en_US
dc.relation.journalApplied Mathematics and Computationen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US


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