Please use this identifier to cite or link to this item: http://bura.brunel.ac.uk/handle/2438/6805
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dc.contributor.authorYamada, T-
dc.contributor.authorKumar, A-
dc.contributor.authorYutaka, A-
dc.contributor.authorFaghri, M-
dc.contributor.author3rd Micro and Nano Flows Conference (MNF2011)-
dc.date.accessioned2012-09-28T15:22:07Z-
dc.date.available2012-09-28T15:22:07Z-
dc.date.issued2011-
dc.identifier.citation3rd Micro and Nano Flows Conference, Thessaloniki, Greece, 22-24 August 2011en_US
dc.identifier.isbn978-1-902316-98-7-
dc.identifier.urihttp://bura.brunel.ac.uk/handle/2438/6805-
dc.descriptionThis paper was presented at the 3rd Micro and Nano Flows Conference (MNF2011), which was held at the Makedonia Palace Hotel, Thessaloniki in Greece. The conference was organised by Brunel University and supported by the Italian Union of Thermofluiddynamics, Aristotle University of Thessaloniki, University of Thessaly, IPEM, the Process Intensification Network, the Institution of Mechanical Engineers, the Heat Transfer Society, HEXAG - the Heat Exchange Action Group, and the Energy Institute.en_US
dc.description.abstractDissipative particle dynamics (DPD) with energy conservation was applied to simulate forced convection in parallel-plate channels with boundary conditions of constant wall temperature (CWT) and constant wall heat flux (CHF). DPD is a coarse-grained version of molecular dynamics. An additional governing equation for energy conservation was solved along with conventional DPD equations where inter-particle heat flux accounts for changes in mechanical and internal energies when particles interact with surrounding particles. The solution domain was considered to be two-dimensional with periodic boundary condition in the flow direction. Additional layers of particles on top and bottom of the channel were utilized to apply no-slip velocity and temperature boundary conditions. The governing equations for energy conservation were modified based on periodic fully developed velocity and temperature conditions. The results were shown via temperature profiles across the channel cross section. The Nusselt numbers were calculated from the temperature gradient at the wall using a second order accurate forward difference technique. The results agreed well with the exact solutions to within 2.3%.en_US
dc.description.sponsorshipThis work is supported by the National Science Foundation grant (NSF-OISE-0530203).en_US
dc.language.isoenen_US
dc.publisherBrunel Universityen_US
dc.subjectDissipative particle dynamicsen_US
dc.subjectEnergy conservationen_US
dc.subjectForced convectionen_US
dc.subjectHeat transferen_US
dc.subjectMicroscaleen_US
dc.subjectMesoscaleen_US
dc.titleForced convection heat transfer simulation using dissipative particle dynamics with energy conservationen_US
dc.typeConference Paperen_US
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