双面薄水平等温板非定常自然对流数值研究

K. Bandyopadhyay, P. Oosthuizen, Qingguo Li
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摘要

本文对复杂形状的双面薄等温水平板突然加热后的非定常自然对流换热进行了数值研究。这些板是等温的,并在环境条件下暴露在空气中。考虑了三种不同的板形。首先用不同瑞利数的努塞尔数在无量纲时间下表示的换热率的变化,以板表面积的平方根作为长度尺度。然后,在相同长度尺度下,得到了稳态换热率。瞬态换热率结果表明,随着瑞利数的增大,努塞尔数要么逐渐减小到稳态值,要么先减小到最小值,然后再增大到稳态值。所考虑的所有板形都得到了相似的努塞尔数随时间的变化。现在,在对不同形状水平板稳态自然对流换热率的研究中发现,如果用4*面积/周长作为表示结果的长度尺度,那么对于所有考虑形状的水平板,努塞尔数与瑞利数的变化基本上是相同的。因此,以4*面积/周长为长度尺度重新表示本研究得到的非定常状态结果,发现以4*面积/周长为长度尺度时,不同瑞利数对所考虑的板形的努塞尔数随无因次时间的变化比以板面积的平方根为长度尺度时更接近。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Numerical Study of Unsteady Natural Convection from Two-Sided Thin Horizontal Isothermal Plates
Unsteady natural convective heat transfer following sudden heating of two-sided, thin isothermal horizontal plates with complex shapes has been numerically studied. The plates were isothermal and exposed to air at ambient conditions. Three different plate shapes were considered. Variations of the heat transfer rates, expressed in terms of the Nusselt number with dimensionless time for various Rayleigh numbers were first obtained with the square root of the plates’ surface area being used as the length scale. Then, the heat transfer rates for steady state were obtained with the same length scale being used. The transient heat transfer rate results showed that depending on the value of the Rayleigh number, the Nusselt number either gradually decreased to a steady state value or first decreased to a minimum and then increased to the steady state value. Similar Nusselt number variation with time were obtained for all plate shapes considered. Now, in studies of steady state natural convective heat transfer rates from horizontal plates with different shapes, it has been found that if 4*Area/Perimeter is used as the length scale in presenting the results, the variation of Nusselt number with Rayleigh number were essentially the same for all shapes considered. Therefore, the unsteady state results obtained in the present study were re-expressed using 4*Area/Perimeter as the length scale and it was found that the variations of Nusselt number with dimensionless time for various Rayleigh numbers for the plate shapes considered, were much closer to each other when 4*area/perimeter was used as the length scale than when the square root of the plate area was used as the length scale.
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