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Law of the wall for a temporally evolving vertical natural convection boundary layer
Abstract The present study concerns a temporally developing parallel natural convection boundary layer with Prandtl number $\textit {Pr} = 0.71$ over an isothermally heated vertical plate. Three-dimensional direct numerical simulations (DNS) with different initial conditions were carried out to inve...
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Published in: | Journal of fluid mechanics 2020-11, Vol.902, Article A31 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Abstract
The present study concerns a temporally developing parallel natural convection boundary layer with Prandtl number
$\textit {Pr} = 0.71$
over an isothermally heated vertical plate. Three-dimensional direct numerical simulations (DNS) with different initial conditions were carried out to investigate the turbulent statistical profiles of mean velocity and temperature up to
${\textit {Gr}}_\delta =7.7\times 10^7$
, where
$Gr_\delta$
is the Grashof number based on the boundary layer thickness
$\delta$
. By virtue of DNS, we have identified a constant heat flux layer (George & Capp,
Intl J. Heat Mass Transfer
, vol. 22, issue 6, 1979, pp. 813–826; Hölling & Herwig,
J. Fluid Mech.
, vol. 541, 2005, pp. 383–397) and a constant forcing layer in the near-wall region. In the close vicinity of the wall (
$y^+50$
), there is a log-law region for the mean temperature profile as reported by Tsuji & Nagano (1988). In this region, the turbulent length scale which characterises mixing scales linearly with the distance from the wall once
${\textit {Gr}}_\delta$
is sufficiently large. By taking the varying buoyancy into consideration with the robust mixing length model, a modified log-law for the mean velocity profile for
$y^+>50$
is proposed. The effect of the initialization is shown to persist until relatively high
${\textit {Gr}}_\delta$
as a result of slow adjustment of the buoyancy (temperature) profile. Once these differences are accounted for, we find excellent agreement with our two DNS cases and with the spatially developing data of Tsuji & Nagano (1988). In the limit of higher
${\textit {Gr}}_\delta$
the velocity profile is expected to become asymptotic to momentum-dominated behaviour as buoyancy becomes increasingly weak in comparison with shear in the near-wall region. |
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ISSN: | 0022-1120 1469-7645 |
DOI: | 10.1017/jfm.2020.621 |