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dc.creatorGrammenos, T.en
dc.creatorGiannakopoulos, A.en
dc.date.accessioned2015-11-23T10:29:09Z
dc.date.available2015-11-23T10:29:09Z
dc.date.issued2014
dc.identifier10.1002/mma.2902
dc.identifier.issn0170-4214
dc.identifier.urihttp://hdl.handle.net/11615/28190
dc.description.abstractA quasicontinuum self-diffusion theory that can capture the fluid ordering effects and density variations predicted by nonequilibrium molecular dynamics in nanochannel flows is presented. The physics of the problem suggests a fourth order diffusion equation for the concentration as a function of position and time requiring the classic diffusion coefficient D and a microstructural internal length g that relates directly to the shape of the molecular potential of the molecular dynamics simulations. Given the appropriate initial and boundary conditions, the aforesaid linear partial differential equation is analytically solved for the one-dimensional steady state, whereas the case of symmetric as well as asymmetric wall conditions has been accounted for by examining different inhomogeneous diffusion distributions. Copyright (c) 2013 John Wiley & Sons, Ltd.en
dc.sourceMathematical Methods in the Applied Sciencesen
dc.source.uri<Go to ISI>://WOS:000328520100008
dc.subjectnanofluidicsen
dc.subjectmolecular dynamicsen
dc.subjectFick's lawsen
dc.subjectdiffusion equationen
dc.subjectMathematics, Applieden
dc.titleFluid ordering effects and density variations in nanochannel flows: a quasicontinuum theoryen
dc.typejournalArticleen


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