Limitations of the background field method applied to Rayleigh-Bénard convection
arXiv:1605.08135 · doi:10.1063/1.5002559
Abstract
We consider Rayleigh-Bénard convection as modeled by the Boussinesq equations, in case of infinite Prandtl number. There is a broad interest in bounds of the upwards heat flux, as given by the Nusselt number , in terms of the forcing via the imposed temperature difference, as given by the Rayleigh number in the turbulent regime . In several works, the background field method applied to the temperature field has been used to provide upper bounds on in terms of . In these applications, the background field method comes in form of a variational problem where one optimizes a stratified temperature profile subject to a certain stability condition; the method is believed to capture marginal stability of the boundary layer. The best available upper bound via this method is ; it proceeds via the construction of a stable temperature background profile that increases logarithmically in the bulk. In this paper, we show that the background temperature field method cannot provide a tighter upper bound in terms of the power of the logarithm. However, by another method one does obtain the tighter upper bound , so that the result of this paper implies that the background temperature field method is unphysical in the sense that it cannot provide the optimal bound.
54 pages, 5 figures, 25 references
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