Direct numerical simulation of inertio-elastic turbulent Taylor–Couette flow. (10th November 2021)

• Record Type: Journal Article
• Authors: Song, Jiaxing; Lin, Fenghui; Liu, Nansheng; Lu, Xi-Yun; Khomami, Bamin
• Is Part Of: Journal of fluid mechanics. Volume 926(2021)
• Publication Date: 2021-11-10
• Subjects: turbulence simulation -- viscoelasticity -- Taylor–Couette flow; Fluid mechanics -- Periodicals; 532.005
• DOI: 10.1017/jfm.2021.757
• Languages: English
• ISSNs: 0022-1120

Abstract

Abstract: Abstract : The flow physics of inertio-elastic turbulent Taylor–Couette flow for a radius ratio of $0.5$ in the Reynolds number ( $Re$ ) range of $500$ to $8000$ is investigated via direct numerical simulation. It is shown that as $Re$ is increased the turbulence dynamics can be subdivided into two distinct regimes: (i) a low $Re \leqslant 1000$ regime where the flow physics is essentially dominated by nonlinear elastic forces and the main contribution to transport and mixing of momentum, stress and energy comes from large-scale flow structures in the bulk region and (ii) a high $Re \geqslant 5000$ regime where inertial forces govern the flow physics and the flow dynamics is mainly governed by small-scale flow structures in the near-wall region. Flow–microstructure coupling analysis reveals that the elastic Görtler instability in the near-wall region is triggered via significant polymer extension and commensurately high hoop stresses. This instability gives rise to small-scale elastic vortical structures identified as elastic Görtler vortices which are present at all $Re$ considered. In fact, these vortices develop herringbone streaks near the inner wall that have a longer average life span than their Newtonian counterparts due to their elastic origin. Examination of the budgets of mean streamwise enstrophy, mean kinetic energy, turbulent kinetic energy and Reynolds shear stress demonstrates that increasing fluid inertia hinders the generation of elastic stresses, leading to a monotonic reduction of the elastic-related effects on the flow physics.