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首页> 外文期刊>International Journal of Heat and Mass Transfer >Steady natural convection in a vertical cylindrical envelope with adiabatic lateral wall
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Steady natural convection in a vertical cylindrical envelope with adiabatic lateral wall

机译:带有绝热侧壁的垂直圆柱形外壳中的自然自然对流

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The natural convection heat transfer and fluid flow in a vertical cylindrical envelope with constant but different temperatures of the two end surfaces and an adiabatic lateral wall was numerically investigated. Apart from some other applications, it serves as a simplified model of the pulse tube of a pulse tube refrigerator. The simulation was conducted for two end wall temperature differences: ΔT_W = 10 and 220 K. For the cases of ΔT_W = 10 K, it is found that the variation patterns of Nu_L vs. Ra_l within the range of L/D = 3-10 are in good consistency with the experimental and theoretical results provided by Catton and Edward for L/D = 0-2.5. The C-E chart is thus extended from L/D = 2.5 to 10. Within the range of Ra_L = 1.1 x 10~5 to 4 x 10~7 the fluid isothermals in both longitudinal and cross-sections exhibit some laminated character, and the convective heat transfer rate is in the same order or one-order larger than that of pure heat conduction. For the" case of large temperature difference (ΔT_W = 220 K) the natural convection in the enclosure is quite strong in that the convective heat transfer rate is about two-orders larger than that of pure heat conduction which occurs when the cold end is placed down. To reduce the loss of cooling capacity of the pulse tube refrigerator, the pulse tube should be positioned with cold end down. Numerical simulation also revealed that the ratio of the axial length, L, to the diameter, D, has effect on the average heat transfer rate of the envelope under the same other conditions. Within the range of L/D = 1-9, the increase in L/D leads to the decrease in heat transfer rate.
机译:数值研究了一个垂直的圆柱形外壳中的自然对流传热和流体流动,该外壳具有恒定但两个端表面和绝热侧壁的温度不同。除了某些其他应用,它还可以作为脉冲管制冷机的脉冲管的简化模型。针对两个端壁温差进行了模拟:ΔT_W= 10和220K。对于ΔT_W= 10 K的情况,发现在L / D = 3-10的范围内Nu_L与Ra_1的变化模式与Catton和Edward提供的L / D = 0-2.5的实验和理论结果高度吻合。因此,CE图从L / D = 2.5扩展到10。在Ra_L = 1.1 x 10〜5到4 x 10〜7的范围内,纵向和横截面的流体等温线都表现出一定的层状特征,并且对流传热速率比纯热传导速率高一个数量级或一个数量级。对于“大温差(ΔT_W= 220 K)的情况”,外壳中的自然对流非常强,因为对流传热速率比放置冷端时发生的纯热传导速率大大约两倍。为了减少脉冲管制冷机的冷却能力损失,应将脉冲管的冷端朝下放置,数值模拟还显示,轴向长度L与直径D的比对在相同的其他条件下,外壳的平均传热速率在L / D = 1-9的范围内,L / D的增加会导致传热速率的降低。

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