dc.contributorUniversidade de São Paulo (USP)
dc.contributorUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2020-12-10T19:35:43Z
dc.date.accessioned2022-12-19T20:13:41Z
dc.date.available2020-12-10T19:35:43Z
dc.date.available2022-12-19T20:13:41Z
dc.date.created2020-12-10T19:35:43Z
dc.date.issued2014-01-01
dc.identifier11th World Congress On Computational Mechanics; 5th European Conference On Computational Mechanics; 6th European Conference On Computational Fluid Dynamics, Vols V - Vi. 08034 Barcelona: Int Center Numerical Methods Engineering, p. 4950-4961, 2014.
dc.identifierhttp://hdl.handle.net/11449/196170
dc.identifierWOS:000485094600031
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/5376807
dc.description.abstractThere exists growing interest in modelling flows at millimetric and micrometric scales, characterised by low Reynolds numbers (Re << 1). In this work, we investigate the performance of projection methods (of the algebraic-splitting kind) for the computation of steady-state simple benchmark problems. The most popular approximate factorization methods are assessed, together with two so-called exact factorization methods. The results show that: (a) The error introduced by non-incremental schemes on the steady state solution is unacceptably large even in the simplest of flows. This is well-known for the basic first order scheme and motivated variants aiming at increased accuracy. Unfortunately, the variants studied either become unstable for the time steps of interest, or yield steady states with larger error than the basic first order scheme. (b) Incremental schemes have an optimal time step delta t* so as to reach the steady state with minimum computational effort. Taking delta t = delta t* the code reaches the steady state in not less than a few hundred time steps. Such a cost is significantly higher than that of solving the velocity-pressure coupled system, which can compute the steady state in one shot. (c) The main difficulty, however, is that if delta t is chosen too large (in general delta t* is not known), then thousands or tens of thousands of time steps are required to reach the numerical steady state with incremental projection methods. The numerical solutions of these methods follow a time-step-dependent spurious transient which makes the computation of steady states prohibitively expensive.
dc.languageeng
dc.publisherInt Center Numerical Methods Engineering
dc.relation11th World Congress On Computational Mechanics; 5th European Conference On Computational Mechanics; 6th European Conference On Computational Fluid Dynamics, Vols V - Vi
dc.sourceWeb of Science
dc.subjectProjection method
dc.subjectNavier-Stokes equations
dc.subjectIncompressible flow
dc.subjectAlgebraic splitting
dc.subjectLow Reynolds number
dc.subjectMicrofluidics
dc.titlePERFORMANCE OF PROJECTION METHODS FOR LOW-REYNOLDS-NUMBER FLOWS
dc.typeActas de congresos


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