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首页> 外文期刊>Journal of Fluid Mechanics >Aspect ratio dependence of heat transport by turbulent Rayleigh- Bénard convection in rectangular cells
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Aspect ratio dependence of heat transport by turbulent Rayleigh- Bénard convection in rectangular cells

机译:矩形单元中湍流瑞利-贝纳德对流对热传输的长宽比依赖性

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We report high-precision measurements of the Nusselt number N as a function of the Rayleigh number $Ra$ in water-filled rectangular Rayleigh-Bénard convection cells. The horizontal length L and width W of the cells are 50.0 and 15.0 cm, respectively, and the heights $H= 49. 9$, 25.0, 12.5, 6.9, 3.5, and 2.4 cm, corresponding to the aspect ratios Γx}=L/ H, Γ y = W/ H)= (1, 0. 3) (2, 0. 6) (4, 1. 2) (7. 3, 2. 2) (14. 3, 4. 3) (20. 8, 6. 3)$. The measurements were carried out over the Rayleigh number range 6 ×10~5 Ra 10~ (11) and the Prandtl number range $5. 2 Pr 7. Our results show that for rectangular geometry turbulent heat transport is independent of the cells' aspect ratios and hence is insensitive to the nature and structures of the large-scale mean flows of the system. This is slightly different from the observations in cylindrical cells where N is found to be in general a decreasing function of Γ $, at least for Γ = 1 and larger. Such a difference is probably a manifestation of the finite plate conductivity effect. Corrections for the influence of the finite conductivity of the top and bottom plates are made to obtain the estimates of Nu∞ for plates with perfect conductivity. The local scaling exponents β} _(-1) of ∞ ~ R~(β-1) are calculated and found to increase from 0.243 at Ra~ 9 × 1~5 to 0.327 at Ra~ 4× 1~(10).
机译:我们报告了在充满水的矩形Rayleigh-Bénard对流池中Nusselt数N随Rayleigh数$ Ra $的函数的高精度测量。单元的水平长度L和宽度W分别为50.0和15.0 cm,高度$ H =49。9 $,25.0、12.5、6.9、3.5和2.4 cm,对应于长宽比Γx} = L / H,Γy = W / H)=(1,0. 3)(2,0. 6)(4,1. 2)(7. 3,2. 2)(14. 3,4. 3) (20. 8,6. 3)$。测量在瑞利数范围6×10〜5 Ra 10〜(11)和普朗特数范围$ 5上进行。 2 Pr7。我们的结果表明,对于矩形几何形状,湍流的热传递与单元的纵横比无关,因此对系统的大规模平均流的性质和结构不敏感。这与圆柱单元中的观察结果略有不同,在圆柱单元中,至少对于Γ= 1或更大,通常发现N是Γ$的递减函数。这种差异可能是有限板电导率效应的体现。对顶板和底板的有限电导率的影响进行校正,以获得具有理想电导率的板的Nu∞估计值。计算了∞〜R〜(β-1)的局部缩放指数β} _(-1),发现它从Ra〜9×1〜5的0.243增加到Ra〜4×1〜(10)的0.327。

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