Applied and Interdisciplinary Mathematics Seminar Friday, September 24, 3:10-4:00pm, 1084 East Hall |
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Abstract |
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Firstly we examine the mean flow structure of isothermal turbulence
in a numerically-simulated square duct at marginal Reynolds number.
The secondary flow in a marginal state exhibits a four-vortex pattern
alternating in time, which is very different from the usual eight-vortex
secondary flow in a fully turbulent state.
It is shown that at the marginal Reynolds number only one pair of
opposite walls can accommodate buffer-layer coherent structures,
i.e., streamwise vortices, leading to the four-vortex mean secondary flow.
We discuss the relevance of this observation with the four-vortex
traveling-wave recently found by Okino, Nagata, Wedin and Bottaro (2010).
Next we move on to the higher-Reynolds-number regime in the thermal turbulent
square-duct flow.
It is found that at higher Reynolds numbers all the walls accommodate
a pair of counter-rotating instantaneous streamwise vortices, so that
the usual eight-vortex secondary flow appears as their statistical footprint.
We can say that the buffer-layer coherent structures play a crucial role in
the appearance of secondary flow of Prandtl's second kind.
We also present the eight-vortex traveling wave which provides a theoretical
support of a direct link between the coherent structures and the
turbulence-driven secondary flow.
Lastly we discuss turbulence- and buoyancy-driven secondary flow in a
numerically-simulated horizontal square duct heated from below.
At moderate Richardson numbers the mean secondary flow is observed to be
represented by a single large-scale thermal convection roll and four
turbulence-driven corner vortices of the opposite sense of rotation
to the roll, as contrasted with the isothermal secondary flow.
This remarkable structural difference in the corner regions can be
interpreted in terms of combined effects, on instantaneous
streamwise vortices, of the large-scale circulation and of the geometrical
constraint by the duct corner.
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