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- W3100495845 endingPage "44005" @default.
- W3100495845 startingPage "44005" @default.
- W3100495845 abstract "By tailoring the geometry of the upper boundary in turbulent Rayleigh-B'enard convection we manipulate the boundary layer -- interior flow interaction, and examine the heat transport using the Lattice Boltzmann method. For fixed amplitude and varying boundary wavelength $lambda$, we find that the exponent $beta$ in the Nusselt-Rayleigh scaling relation, $Nu-1 propto Ra^beta$, is maximized at $lambda equiv lambda_{text{max}} approx (2 pi)^{-1}$, but decays to the planar value in both the large ($lambda gg lambda_{text{max}}$) and small ($lambda ll lambda_{text{max}}$) wavelength limits. The changes in the exponent originate in the nature of the coupling between the boundary layer and the interior flow. We present a simple scaling argument embodying this coupling, which describes the maximal convective heat flux." @default.
- W3100495845 created "2020-11-23" @default.
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- W3100495845 date "2015-08-01" @default.
- W3100495845 modified "2023-09-27" @default.
- W3100495845 title "Tailoring boundary geometry to optimize heat transport in turbulent convection" @default.
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- W3100495845 doi "https://doi.org/10.1209/0295-5075/111/44005" @default.
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