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Effect of Large-Scale Flow on the Boundary Layer Velocity Field in Turbulent Convection

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In this article, the effect of shear on the boundary layers on the hot plate in Rayleigh-Benard convection for a range of Prandtl numbers 4.69 ≤ Pr ≤ 5.88 and Rayleigh numbers 105 ≤ Ra ≤ 109 was studied.
Abstract
We study the effect of shear by the inherent large-scale flow in the bulk on the boundary layers on the hot plate in Rayleigh–Benard convection for a range of Prandtl numbers 4.69 ≤ Pr ≤ 5.88 and Rayleigh numbers 105 ≤ Ra ≤ 109. We observe that, at each Ra, at an instant, the distribution of horizontal velocities within the boundary layer in a horizontal plane is either of a unimodal nature or of a bimodal nature. Unimodal distributions occur either at low Ra or at high Ra while the bimodal distributions occur more at intermediate Ra. The peak of the unimodal distribution at low Ra occurs at values at around Vbl, the natural convection boundary layer velocity while the peak of the unimodal PDFs at high Ra occur at values greater than or equal to Vsh, the large-scale flow velocity. In the case of bimodal distributions, the first peak occurs in between Vbl and Vsh while the second peak occurs after Vsh. We show that the second peak of the bimodal distribution and the unimodal peak which occur at ≥Vsh scales as Vsh scales with Ra. The first peak of bimodal distribution and the single peak occurring at around Vbl scales with Ra as the natural convection boundary layer velocity forced by shear.

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Journal ArticleDOI

Effect of shear on local boundary layers in turbulent convection

TL;DR: In this article , the effect of shear by the inherent large-scale flow (LSF) on the local boundary layers on the hot plate was studied, and it was shown that the velocities in the remaining regions, which contribute to the first peak of the bimodal type B distributions and the single peak of type A distributions, are also affected by the shear.
References
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Journal ArticleDOI

Heat transfer and large scale dynamics in turbulent Rayleigh-Bénard convection

TL;DR: In this article, the Nusselt number and the Reynolds number depend on the Rayleigh number Ra and the Prandtl number Pr, and the thicknesses of the thermal and the kinetic boundary layers scale with Ra and Pr.
Journal ArticleDOI

Scaling of hard thermal turbulence in Rayleigh-Bénard convection

TL;DR: In this article, an experimental study of Rayleigh-Benard convection in helium gas at roughly 5 K is performed in a cell with aspect ratio 1.65 and 1.5.
Journal ArticleDOI

Steady laminar natural convection plumes above a horizontal line heat source

TL;DR: In this paper, a simple formulation of the boundary value problem for a wide range of values of the Prandtl number has been proposed, and results of experiments with plumes are included to emphasize the various properties of plume flow and to indicate that the large thickness of boundary region in the range of stable laminar plumes (i.e. at relatively low local Grashof numbers) should encourage the calculation of higher order approximate of the flow.
Journal ArticleDOI

Plume structure in high-Rayleigh-number convection

TL;DR: In this paper, the authors show that the near-wall structure is made of laminar natural-convection boundary layers, which become unstable to give rise to sheet plumes, and conclude that in the presence of a mean wind, the local nearwall boundary layers associated with each sheet plume in high-rayleigh-number turbulent natural convection are likely to be Laminar mixed convection type.
Journal ArticleDOI

On the stability of natural convection boundary layer flow over horizontal and slightly inclined surfaces

TL;DR: In this paper, the stability of a natural convection boundary layer flow adjacent to horizontal and to slightly inclined surfaces was analyzed using a Mach-Zehnder interferometer, and the results of a perturbation analysis of such flows were used to study flow characteristics under both disturbed and undisturbed conditions.
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