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Investigation of natural circulation in cavities with uniform heat generation for different Prandtl number fluids

机译:不同普朗特数流体在均匀发热的腔体内自然循环的研究

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Natural convection in enclosures with uniform heat generation and isothermal side walls is studied here. For the rectangular enclosure, two-dimensional conservation equations are solved using SIMPLE algorithm. Parametric studies are conducted to examine the effects of orientation of the cavity, fluid properties (Pr number), and aspect ratio for Rayleigh numbers up to 10~6. For a horizontal square cavity, the flow becomes periodically oscillating at Rα = 5 × 10~4 and chaotic at Rα = 8 × 10~5. With a slight increase in the inclination angle, the oscillations die and for inclination angles greater than 15°, the flow attain a steady state over a range of Ra. It is found that for tall cavities (aspect ratio < 1), the steady-state solution is obtained for all values of Ra considered here. However, for wide cavities (aspect ratio < 1), an oscillatory flow regime is observed. The maximum temperature within the cavity is calculated for the range of Ra, aspect ratio and Pr number. Correlations for the maximum cavity temperature is presented here. The values of critical Rayleigh number at which the convection sets in the rectangular cavity are also studied and two distinct criteria are determined to evaluate the critical Rayleigh number. Further, a three-dimensional simulation is performed for a cubic cavity. It is found that the steady state solutions are obtained for all Rayleigh number, except at Ra = 10~6. This is in contrast to the predictions for a two-dimensional square cavity, which has an oscillatory zone from Rα = 5 × 10~4 onwards.
机译:在这里研究了均匀热量产生和等温侧壁的外壳中的自然对流。对于矩形外壳,使用SIMPLE算法求解二维守恒方程。进行了参数研究,以检查腔的方向,流体特性(Pr值)和高达10〜6的瑞利数的长宽比的影响。对于水平方腔,流动在Rα= 5×10〜4时周期性振荡,在Rα= 8×10〜5时混沌。随着倾斜角的略微增加,振荡消失,并且对于大于15°的倾斜角,流在Ra范围内达到稳定状态。结果发现,对于高空洞(长径比<1),对于此处考虑的所有Ra值均获得稳态解。但是,对于宽腔(宽高比<1),观察到振荡流动状态。计算腔内的最高温度是针对Ra,纵横比和Pr数的范围。此处显示了最大腔体温度的相关性。还研究了矩形腔中对流集的临界瑞利数值,并确定了两个不同的标准来评估临界瑞利数。此外,对立方腔进行三维模拟。结果发现,除了Ra = 10〜6以外,所有瑞利数都可以得到稳态解。这与二维方腔的预测相反,后者具有从Rα= 5×10〜4开始的振荡区域。

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