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Space–time dynamics of optimal wavepackets for streaks in a channel entrance flow

Article dans une revue avec comité de lecture
Author
ALIZARD, Frédéric
134975 Laboratoire de Dynamique des Fluides [DynFluid]
CADIOU, A.
694 Laboratoire de Mecanique des Fluides et d'Acoustique [LMFA]
LE PENVEN, L.
694 Laboratoire de Mecanique des Fluides et d'Acoustique [LMFA]
DI PIERRO, B.
694 Laboratoire de Mecanique des Fluides et d'Acoustique [LMFA]
BUFFAT, M.
694 Laboratoire de Mecanique des Fluides et d'Acoustique [LMFA]

URI
http://hdl.handle.net/10985/18898
DOI
10.1017/jfm.2018.191
Date
2018
Journal
Journal of Fluid Mechanics

Abstract

The laminar–turbulent transition of a plane channel entrance flow is revisited using global linear optimization analyses and direct numerical simulations. The investigated case corresponds to uniform upstream velocity conditions and a moderate value of Reynolds number so that the two-dimensional developing flow is linearly stable under the parallel flow assumption. However, the boundary layers in the entry zone are capable of supporting the development of streaks, which may experience secondary instability and evolve to turbulence. In this study, global optimal linear perturbations are computed and studied in the nonlinear regime for different values of streak amplitude and optimization time. These optimal perturbations take the form of wavepackets having either varicose or sinuous symmetry. It is shown that, for short optimization times, varicose wavepackets grow through a combination of Orr and lift-up effects, whereas for longer target times, both sinuous and varicose wavepackets exhibit an instability mechanism driven by the presence of inflection points in the streaky flow. In addition, while the optimal varicose modes obtained for short optimization times are localized near the inlet, where the base flow is strongly three-dimensional, when the target time is increased, the sinuous and varicose optimal modes are displaced farther downstream, in the nearly parallel streaky flow. Finally, the optimal wavepackets are found to lead to turbulence for sufficiently high initial amplitudes. It is noticed that the resulting turbulent flows have the same wall-shear stress, whether the wavepackets have been obtained for short or for long time optimization.

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