an:07116506
Zbl 1430.76223
Pereira, Anselmo S.; Thompson, Roney L.; Mompean, Gilmar
Common features between the Newtonian laminar-turbulent transition and the viscoelastic drag-reducing turbulence
EN
J. Fluid Mech. 877, 405-428 (2019).
00440195
2019
j
76F06 76A10 76F70
drag reduction; viscoelasticity; turbulent transition
Summary: The transition from laminar to turbulent flows has challenged the scientific community since the seminal work of \textit{O. Reynolds} [Philos. Trans. R. Soc. Lond. 174, 935-982 (1883; JFM 16.0845.02)]. Recently, experimental and numerical investigations on this matter have demonstrated that the spatio-temporal dynamics that are associated with transitional flows belong to the directed percolation class. In the present work, we explore the analysis of laminar-turbulent transition from the perspective of the recent theoretical development that concerns viscoelastic turbulence, i.e. the drag-reducing turbulent flow obtained from adding polymers to a Newtonian fluid. We found remarkable fingerprints of the variety of states that are present in both types of flows, as captured by a series of features that are known to be present in drag-reducing viscoelastic turbulence. In particular, when compared to a Newtonian fully turbulent flow, the universal nature of these flows includes: (i) the statistical dynamics of the alternation between active and hibernating turbulence; (ii) the weakening of elliptical and hyperbolic structures; (iii) the existence of high and low drag reduction regimes with the same boundary; (iv) the relative enhancement of the streamwise-normal stress; and (v) the slope of the energy spectrum decay with respect to the wavenumber. The maximum drag reduction profile was attained in a Newtonian flow with a Reynolds number near the boundary of the laminar regime and in a hibernating state. It is generally conjectured that, as the Reynolds number increases, the dynamics of the intermittency that characterises transitional flows migrate from a situation where heteroclinic connections between the upper and the lower branches of solutions are more frequent to another where homoclinic orbits around the upper solution become the general rule.
JFM 16.0845.02