Abstract

We report the results of an experimental investigation into the decay of turbulence in plane Couette–Poiseuille flow using ‘quench’ experiments where the flow laminarises after a sudden reduction in Reynolds number $Re$ . Specifically, we study the velocity field in the streamwise–spanwise plane. We show that the spanwise velocity containing rolls decays faster than the streamwise velocity, which displays elongated regions of higher or lower velocity called streaks. At final Reynolds numbers above $425$ , the decay of streaks displays two stages: first a slow decay when rolls are present and secondly a more rapid decay of streaks alone. The difference in behaviour results from the regeneration of streaks by rolls, called the lift-up effect. We define the turbulent fraction as the portion of the flow containing turbulence and this is estimated by thresholding the spanwise velocity component. It decreases linearly with time in the whole range of final $Re$ . The corresponding decay slope increases linearly with final $Re$ . The extrapolated value at which this decay slope vanishes is $Re_{a_z}\approx 656\pm 10$ , close to $Re_g\approx 670$ at which turbulence is self-sustained. The decay of the energy computed from the spanwise velocity component is found to be exponential. The corresponding decay rate increases linearly with $Re$ , with an extrapolated vanishing value at $Re_{A_z}\approx 688\pm 10$ . This value is also close to the value at which the turbulence is self-sustained, showing that valuable information on the transition can be obtained over a wide range of $Re$ .

Highlights

  • The transition to turbulence is complex in wall-bounded shear flows

  • Even if the noise is small in amplitude, the transition to turbulence occurs at values of Re that are finite and lower than the theoretical linear critical Reynolds number Rel, which is infinite for plane Couette flow (PCF) and Couette-Poiseuille flow (CPF) with zero mean flow (Klotz & Wesfreid 2017)

  • We have investigated the decay of turbulence in Couette-Poiseuille flow using quench experiments

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Summary

Introduction

The transition to turbulence is complex in wall-bounded shear flows. Examples include plane Couette flow (PCF), plane Poiseuille flow (PPF) and Couette-Poiseuille flow (CPF). The global threshold obtained numerically is Reg = 700 (Shimizu & Manneville 2019) This is consistent with the experimental results of PPF by Paranjape (2019) where a positive mean growth rate of the turbulent bands for Re > 650 is found in quench experiments (Bottin & Chate 1998; De Souza et al 2020). By way of contrast with PCF, the crossover Reynolds number obtained by equating the decay and splitting rate in a tilted narrow channel (Re = 965, see the numerical work by Gome et al (2020)) is different from Reg. Since the mean flux is approximately zero in our experiment we use the belt speed Ubelt as the characteristic velocity. We studied four levels of external noise: one without the grid (high noise) and three with the grid in place

Particle image velocimetry
Protocol
Small scales
Energy and turbulent fraction
Decay process
External noise in the permanent regime
Advection of turbulent spots
Intrinsic noise
Variation of characteristic times with Ref
Findings
Conclusion
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