Polymer-laden turbulent pipe flows are investigated through direct numerical simulations with Lagrangian transport, and back reaction, of 10 8 polymers, modelled as FENE dumbbells. A wide range Weissenberg number (Wi) comparison with results obtained via the FENE-P model shows quantitative and qualitative discrepancies between the two models. It is shown that the relevant hypothesis that fails and causes the differences is Peterlin’s approximation, leading to unphysical polymer extensions and thus back reaction. A new parameter, the polymer Reynolds number Re p is defined. At fixed Re p and Re, the dynamics depends only on Wi and not on the individual polymer parameters, i.e. friction coefficient gamma, contour length L, and concentration c o , entering in Re p. Alongside the increase in available computational power, this finding allows reducing drastically the cost of Lagrangian simulations, since c o, gamma, and L can be interchanged, and propose the FENE model as a valuable alternative to the well-established, and meritorious, FENE-P model.
The role of polymer parameters and configurations in drag-reduced turbulent wall-bounded flows: Comparison between FENE and FENE-P / Serafini, F.; Battista, F.; Gualtieri, P.; Casciola, C. M.. - In: INTERNATIONAL JOURNAL OF MULTIPHASE FLOW. - ISSN 0301-9322. - 165:(2023). [10.1016/j.ijmultiphaseflow.2023.104471]
The role of polymer parameters and configurations in drag-reduced turbulent wall-bounded flows: Comparison between FENE and FENE-P
Serafini, F.
Primo
;Battista, F.Secondo
;Gualtieri, P.Penultimo
;Casciola, C. M.
Ultimo
2023
Abstract
Polymer-laden turbulent pipe flows are investigated through direct numerical simulations with Lagrangian transport, and back reaction, of 10 8 polymers, modelled as FENE dumbbells. A wide range Weissenberg number (Wi) comparison with results obtained via the FENE-P model shows quantitative and qualitative discrepancies between the two models. It is shown that the relevant hypothesis that fails and causes the differences is Peterlin’s approximation, leading to unphysical polymer extensions and thus back reaction. A new parameter, the polymer Reynolds number Re p is defined. At fixed Re p and Re, the dynamics depends only on Wi and not on the individual polymer parameters, i.e. friction coefficient gamma, contour length L, and concentration c o , entering in Re p. Alongside the increase in available computational power, this finding allows reducing drastically the cost of Lagrangian simulations, since c o, gamma, and L can be interchanged, and propose the FENE model as a valuable alternative to the well-established, and meritorious, FENE-P model.File | Dimensione | Formato | |
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