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倾斜壁面汽泡脱离行为的实验研究OA北大核心CSTPCD

Experimental Investigation of Bubble Departure Manners at Inclined Heated Wall

中文摘要英文摘要

为探索壁面沸腾过程汽泡的脱离规律,通过可视化实验对倾斜壁面汽泡的脱离行为进行研究,获得了倾斜壁面汽泡主要发生的 3类脱离行为,包括自由脱离、碰撞脱离与扰动脱离.为降低汽泡行为随机性带来的干扰,建立了量化汽泡脱离特征量的最小无关数原则,确定汽泡自由脱离、碰撞脱离的最小无关数分别为 25、34,确保对应脱离特征量的统计偏差小于±5%.在实验参数范围内,基于最小无关数原则统计获得汽泡脱离特征量,结果表明,随着加热壁面热流密度的升高,汽泡自由脱离直径呈增大趋势,汽泡碰撞脱离直径呈减小趋势,汽泡生长时间与等待时间减少,汽泡脱离频率增大.碰撞脱离对汽泡生长时间的减少效应强于对等待时间的延迟效应,综合结果为碰撞脱离缩短了汽泡脱离周期,加快了壁面核化过程.

The visual experimental facility of inclined heated surface was built and the visual experiments in subcooled flow boiling were performed.The results show that there are mainly three manners of bubble departure at one nucleation site,including bubble free departure,bubble collision departure and bubble disturbance departure.Bubble free departure means the objective bubble grows to a specific size and departs from the nucleation site without any influence of other bubbles.It is believed the reason of bubble free departure is that the bubble cannot maintain a static state and continue to grow at the critical size.The bubble will slide along the heated surface after departure.Bubble collision departure means the objective bubble touches other sliding bubbles and merges into a new bubble which will depart from the nucleation site immediately.Bubble disturbance departure means the objective bubble is disturbed by other sliding bubble,but does not recombine with the sliding bubble,and gradually leaves the nucleation site.The minimum irrelevant number rule was established for the quantification of bubble detachment characteristics in order to reduce the interference of randomicity.The minimum irrelevant numbers of bubble free departure and bubble collision departure are 25 and 34 respectively.The statistical errors of bubble departure characteristic quantities are guaranteed within±5%by the minimum irrelevant number rule.Under the minimum irrelevant number rule,the test experiments show that with the increase of heat flux on the heating wall,the bubble free departure diameter increases,the bubble collision departure diameter decreases,the bubble growth time and waiting time decrease,and the bubble departure frequency increases.These indicate that in these experimental conditions,the bubble growth time of bubble collision departure is fully smaller than that of bubble free departure.When collision departure happens,the growing bubble departs earlier owing to the push of sliding bubble,which causes the bubble growth time becomes shorter.This suggests that the bubble waiting time of bubble collision departure is almost larger than that of bubble free departure.In the process of bubble collision departure,a fast-moving sliding bubble knocks into the growing bubble and the newly formed bubble departs from the nucleation site quickly.The collision of sliding bubble and the movement of newly formed bubble disturb the boundary layer near nucleation site seriously,which causes the nucleation site spends a longer time nucleating a bubble renewedly.These results show that the bubble departure frequency of bubble collision departure is fully larger than that of bubble free departure.The reducing effect on bubble growth time is stronger than the delayed effect on bubble waiting time during the process of bubble collision departure,which indicates that bubble collision departure shortens bubble departure cycle and quickens bubble departure process.

肖仁杰;闫晓;昝元锋

中国核动力研究设计院,四川成都 610213

核科学

倾斜壁面汽泡自由脱离汽泡碰撞脱离汽泡扰动脱离脱离直径

inclined heated wallbubble free departurebubble collision departurebubble disturbance departuredeparture diameter

《原子能科学技术》 2024 (007)

1532-1539 / 8

10.7538/yzk.2023.youxian.0890

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