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Film Condensation of Steam Flowing Downward on a Tier of Horizontal Cylinders at Different Inclination Angles in the Presence of a Non-condensable Gas

机译:在不可凝聚的气体存在下,在不同倾斜角度下在水平圆柱体上向下流动的蒸汽缩合

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The problem of forced laminar film condensation of steam flowing downward a tier of horizontal cylinders is investigated numerically. The effects of free stream non-condensable gas,air concentration (m_(1,∞)), free stream velocity (Reynolds number), cylinder diameter, and angle of inclination on the condensation heat transfer are analyzed. Two flow arrangements, inline and staggered, are analyzed and investigated. The mathematical model takes into account the effect of staggering of the cylinders and how condensation is affected at the lower cylinders when condensate does not fall on to the center line of the cylinders. Condensation heat transfer results are available in ranges from (U_∞ = 1 - 30 m/s) for free stream velocity, (m_(1,∞) = 0.01 -0.8) for free stream air mass fraction and (D = 12.7 -50.8 mm) for cylinder diameter. Results show that; a remarked reduction in the vapor side heat transfer coefficient is noticed. This results from the presence of small amounts of free stream air mass fractions in the steam-air mixture and increase in the cylinder diameter. On the other hand, it increases by increasing the free stream velocity (Reynolds number). Average heat transfer coefficient at the middle and the bottom cylinders increases by increasing the angle of inclination, whereas, no significant change is observed for that of the upper cylinder. Down the bank, a rapid decrease in the vapor side heat transfer coefficient is noticed. It may be resulted from the combined effects of inundation, decrease in the vapor velocity and increase in the non-condensable gas (air) at the bottom cylinders in the bank.
机译:在数值上研究了向下流动的蒸汽的强制层膜膜冷凝的问题。分析了游离流不可冷凝气体,空气浓度(M_(1,∞)),自由流速度(雷诺数),气缸直径和倾斜角度的效果。分析和研究了两个流量排列,内联和交错。数学模型考虑了气缸的惊人的效果以及当冷凝物不落在气缸的中心线时,在下汽缸处受到凝结的影响。冷凝传热结果可用于自由流速度的(U_∞= 1-30m / s)的范围,(M_(1,∞)= 0.01-0.8),用于自由流空气质量分数和(d = 12.7 -50.8 mm)用于气缸直径。结果表明注意到蒸汽侧传热系数的评论减少。这是由蒸汽空气混合物中存在少量的自由流空气质量级分,并增加汽缸直径。另一方面,它通过增加自由流速度(雷诺数)而增加。通过增加倾斜角度,底部汽缸在中间和底缸上的平均传热系数增加,而没有针对上圆筒的角度观察到显着变化。向下储存,注意到蒸汽侧传热系数的快速降低。由于淹没的组合效应,储气的血液速度和底部气缸中的不可冷凝气体(空气)的增加而导致。

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