Bounds on vertical heat transport for infinite-Prandtl-number Rayleigh–Bénard convection

Bounds on vertical heat transport for infinite-Prandtl-number Rayleigh–Bénard convection
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DOI:
10.1017/s0022112006000097
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发表时间:
2005-11
影响因子:
3.7
通讯作者:
C. Doering;F. Otto;Maria G. Reznikoff
C. Doering;F. Otto;Maria G. Reznikoff
中科院分区:
工程技术2区
文献类型:
--
作者:
C. Doering;F. Otto;Maria G. Reznikoff

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For the infinite-Prandtl-number limit of the Boussinesq equations, the enhancement of vertical heat transport in Rayleigh–Bénard convection, the Nusselt number $\hbox{\it Nu}$, is bounded above in terms of the Rayleigh number $\hbox{\it Ra}$ according to $\hbox{\it Nu}\,{\le}\,0.644 \,{\times}\hbox{\it Ra}^{{1}/{3}} [\log{\hbox{\it Ra}}]^{{1}/{3}}$ as $\hbox{\it Ra}\,{\rightarrow}\,\infty$. This result follows from the utilization of a novel logarithmic profile in the background method for producing bounds on bulk transport, together with new estimates for the bi-Laplacian in a weighted $L^{2}$ space. It is a quantitative improvement of the best currently available analytic result, and it comes within the logarithmic factor of the pure 1/3 scaling anticipated by both the classical marginally stable boundary layer argument and the most recent high-resolution numerical computations of the optimal bound on $\hbox{\it Nu}$ using the background method.
For the infinite-Prandtl-number limit of the Boussinesq equations, the enhancement of vertical heat transport in Rayleigh–Bénard convection, the Nusselt number $\hbox{\it Nu}$, is bounded above in terms of the Rayleigh number $\hbox{\it Ra}$ according to $\hbox{\it Nu}\,{\le}\,0.644 \,{\times}\hbox{\it Ra}^{{1}/{3}} [\log{\hbox{\it Ra}}]^{{1}/{3}}$ as $\hbox{\it Ra}\,{\rightarrow}\,\infty$. This result follows from the utilization of a novel logarithmic profile in the background method for producing bounds on bulk transport, together with new estimates for the bi-Laplacian in a weighted $L^{2}$ space. It is a quantitative improvement of the best currently available analytic result, and it comes within the logarithmic factor of the pure 1/3 scaling anticipated by both the classical marginally stable boundary layer argument and the most recent high-resolution numerical computations of the optimal bound on $\hbox{\it Nu}$ using the background method.