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- W2912386096 abstract "Logarithmic boundary layers have been observed in different regions in turbulent Rayleigh–Bénard convection (RBC). However, how thermal plumes correlate with the logarithmic law of temperature and how the velocity profile changes with pressure gradient are not fully understood. Here, we perform three-dimensional (3D) simulations of turbulent Rayleigh–Bénard convection in a slim box without the front and back walls, with aspect ratio $$mathrm {width}{:}mathrm {depth}{:}mathrm {height}=L{:}D{:}H=1{:}1/6{:}1$$ (corresponding to the x, y, and z coordinates, respectively), in the Rayleigh number $${Ra} = [1times 10^8, 1times 10^{10}]$$ for Prandtl number $${Pr}=0.7$$ . To investigate the structures of the viscous and thermal boundary layers, we examine the velocity profiles in the streamwise and vertical directions (i.e. U and W) along with the mean temperature profile throughout the plume-impacting, plume-ejecting, and wind-shearing regions. The velocity profile is successfully quantified by a two-layer function of a stress length,, $$ell _u^+ = ell _0^+(z^+)^{3/2} left[ 1+left( {z^+}/{z_mathrm{sub}^+}right) ^4right] ^{1/4}$$ , as proposed by She et al. (J Fluid Mech, 2017), though it is neither Prandtl–Blasius–Pohlhausen (PBP) type nor logarithmic. In contrast, the temperature profile in the plume-ejecting region is logarithmic for all simulated cases, attributed to the emission of thermal plumes. The coefficient of the temperature log law, A, can be described by the composition of the thermal stress length $$ell ^*_{theta 0}$$ and the thicknesses of thermal boundary layer $$z^*_mathrm{sub}$$ and $$z^*_mathrm{buf}$$ , i.e. $$A simeq z^*_mathrm{sub}/left( ell ^*_{theta 0}{z^*_mathrm{buf}}^{3/2}right) $$ . The adverse pressure gradient responsible for turning the wind direction contributes to intensively emitting plumes and the logarithmic temperature profile at the plume-ejecting region. The Nusselt number scaling and the local heat flux in the slim box are consistent with previous results for confined cells. Therefore, the slim-box RBC is a preferred system for investigating in-box kinetic and thermal structures of turbulent convection with the large-scale circulation in a fixed plane." @default.
- W2912386096 created "2019-02-21" @default.
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- W2912386096 date "2019-06-05" @default.
- W2912386096 modified "2023-09-24" @default.
- W2912386096 title "Boundary layer structure in turbulent Rayleigh–Bénard convection in a slim box" @default.
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- W2912386096 doi "https://doi.org/10.1007/s10409-019-00874-x" @default.
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