首页> 外文期刊>Heat Transfer Research >EXPERIMENTAL INVESTIGATION OF AXIAL HEAT TRANSFER AND ENTRANCE EFFECT IN RANDOMLY PACKED BEDS BY A NAPHTHALENE SUBLIMATION TECHNIQUE
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EXPERIMENTAL INVESTIGATION OF AXIAL HEAT TRANSFER AND ENTRANCE EFFECT IN RANDOMLY PACKED BEDS BY A NAPHTHALENE SUBLIMATION TECHNIQUE

机译:萘升华技术在随机包装床中轴向传热和入射效应的实验研究

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摘要

Local average heat transfer characteristics along the axial direction in randomly packed beds are investigated experimentally by using a naphthalene sublimation technique and the heat-to-mass transfer analogy. Packed beds of three particle diameters of 12 mm, 10 mm, and 8 mm are investigated, respectively. The relationship between the Nusselt number along the axial direction and the axial porosity distribution is analyzed, and the influence of the entrance effect on the overall heat transfer is explored. In the present paper, the axial porosity distribution is obtained by numerical analysis of a randomly packed bed generated by a discrete element method (DEM). The results of pressure drop show that most experimental points lie within +/- 20% deviations of the Ergun equation and that the pressure distribution along the axial direction decreases almost linearly. Furthermore, it is found that in the axial direction, the Nusselt number increases in the first three layers and stays almost constant after that, where the heat transfer is fully developed. The development of Nusselt number along the axial direction can be attributed to the change of axial porosity distribution and to the alterative turbulence. Besides, the Nusselt number in the first layer is about 60-80% of the average Nusselt number in the bulk of the packed bed in the present Reynolds number range (373-2867). Finally, the entrance effect can have an influence on the overall Nusselt number when the packed bed is shorter than 8-16 particle diameters.
机译:通过使用萘升华技术和热量传递比较实验研究沿随机包装床中的轴向方向的局部平均传热特性。研究了三个粒径为12毫米,10毫米和8毫米的填充床。分析了沿轴向和轴向孔隙率分布之间的冲泡数与轴向孔隙率分布之间的关系,并且探讨了入射效应对整体传热的影响。在本文中,通过由离散元件方法(DEM)产生的随机包装床的数值分析来获得轴向孔隙孔隙率分布。压降结果表明,大多数实验点位于ERGUN方程的+/- 20%偏差内,并且沿轴向的压力分布几乎线性地减小。此外,发现在轴向方向上,在前三层中的露珠数增加,并且在此之后几乎持续地保持在那里,热传递完全开发。沿轴向的露天数的开发可以归因于轴向孔隙率分布的变化和改变湍流。此外,第一层中的露珠数是本雷诺数范围(373-2867)中的填充床的大部分填充床中的平均冲击数的60-80%。最后,当填充床短于8-16粒径时,入射效应可能对整个露珠数产生影响。

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