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A qualitative assessment of the role of a viscosity depending on the third invariant of the rate-of-deformation tensor upon turbulent non-Newtonian flow
Institution:1. Departamento de Engenharia Electromecânica, Universidade da Beira Interior, Rua Marquês D''Ávila e Bolama, 6200 Covilhã, Portugal;2. Departamento de Engenharia Mecânica e Gestão Industrial, Faculdade de Engenharia, Rua dos Bragas, 4099 Porto Codex, Portugal;1. School of Mathematics and Information Science, North China University of Water Resources and Electric Power, Zhengzhou 450011, China;2. School of Science, Henan University of Engineering, Zhengzhou 451191, China;1. Dipartimento di Matematica, Università di Pisa, Italy;2. Département d''Informatique, Université libre de Bruxelles, Belgium;1. Department of Mathematics and Applications “R. Caccioppoli”, University of Naples Federico II, via Cinthia – Complesso Universitario Monte Sant''Angelo, 80126 Naples, Italy;2. Aix Marseille Univ., CNRS, Centrale Marseille, I2M, Marseille, France;3. Université de Limoges, Laboratoire XLIM, UMR-CNRS 6172, France;4. Centre for Informatics and Applied Optimization, Federation University, Australia;1. Faculty of Mathematics and Statistics, Central China Normal University, PR China;2. Department of Statistics, Visva-Bharati University, Santiniketan, India
Abstract:The numerical simulation of some non-Newtonian effects in wall and wall-free turbulent flows, such as drag reduction in pipe flows or the decrease in transverse normal Reynolds stresses, has been attempted in the past with a limited degree of success on the basis of modified wall functions applied to traditional turbulence models (kε), rather than through more realistic rheological constitutive equations. In this work, it is qualitatively shown that if the viscosity function of a generalised Newtonian fluid is assumed to depend on the third invariant of the rate of deformation tensor, there is an increase of the viscous diffusion terms, but especially, of the dissipation of turbulence kinetic energy by a factor equal to the Trouton ratio of the fluid, divided by the Trouton ratio of the solvent, thus indicating a possible way to improve rheological–turbulence modelling.
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