Bulletin of the American Physical Society
71st Annual Meeting of the APS Division of Fluid Dynamics
Volume 63, Number 13
Sunday–Tuesday, November 18–20, 2018; Atlanta, Georgia
Session E29: Environmental Flows II
5:10 PM–6:28 PM,
Sunday, November 18, 2018
Georgia World Congress Center
Room: B401
Chair: Alain Pumir, Ecole Normale Superieure
Abstract ID: BAPS.2018.DFD.E29.4
Abstract: E29.00004 : Direct Numerical Simulations of Non-linear Time Periodic Flows in a Planar Channel
5:49 PM–6:02 PM
Presenter:
Celalettin Emre Ozdemir
(Louisiana State University)
Authors:
Celalettin Emre Ozdemir
(Louisiana State University)
Soroush Sororian
(Louisiana State University)
Daniel Oliviera
(Louisiana State University)
Ling Zhu
(Northeastern University)
Sahar Haddadian
(Louisiana State University)
Henok Kefelegn
(Louisiana State University)
Christopher Turnipseed
(Louisiana State University)
Details of understanding non-linear time-periodic wall flows are of interest to engineering applications in biomedical and environmental flows. Non-linearity in wall-bounded time-periodic flows, due to higher frequency contribution to the velocity and/or acceleration in the outer layer, significantly alters the wall turbulence. The most striking example is the formation of a net current in the opposite direction of the wave propagation. Here, we present the results of direct numerical simulations of a flow over a smooth wall, driven by a Stokes Second-order Wave (SOSW). Channel flow driven by SOSW has a skewed velocity but symmetric acceleration in the outer region. This allows us investigate the role of velocity skewness to the wall turbulence. Our results suggest that the velocity skewness in the outer region leads to a skewness in the friction velocity and the viscous length scale. The difference of viscous length scale, between the crest and the trough of the wall shear stress, creates a wall-normal offset in Reynolds shear stress during the positive and negative flow. This gives a net Reynolds shear stress, if integrated over a cycle, and creates a net flow. How net flow characteristics changes with respect to Reynolds number is further discussed in this presentation.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DFD.E29.4
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