蒸发热水塔内固体颗粒对气泡运动的影响

胡晨辉; 王亦飞; 包泽彬; 于广锁

doi:10.11949/j.issn.0438-1157.20180697

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蒸发热水塔内固体颗粒对气泡运动的影响

流体力学与传递现象 | 更新时间：2020-06-24

- 蒸发热水塔内固体颗粒对气泡运动的影响
- Effect of solid particles in evaporative hot water tower on bubble movement
- 化工学报 2019年70卷第1期页码：39-48
- 作者机构：
  
  华东理工大学洁净煤技术研究所，煤气化及能源化工教育部重点实验室，上海 200237
- 作者简介：
  
  胡晨辉（1993—），男，硕士研究生，18855587097@163.com
  王亦飞（1970—），女，教授，wangyf@ecust.edu.cn
- 基金信息：
  
  国家重点研发计划项目(2017YFB0602802)
- DOI：10.11949/j.issn.0438-1157.20180697
  中图分类号： TQ 026.2
- 收稿：2018-06-26，
  
  修回：2018-09-30，
  
  纸质出版：2019-01-05
- 稿件说明：
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胡晨辉, 王亦飞, 包泽彬, 于广锁. 蒸发热水塔内固体颗粒对气泡运动的影响[J]. 化工学报, 2019, 70(1): 39-48

HU Chenhui, WANG Yifei, BAO Zebin, YU Guangsuo. Effect of solid particles in evaporative hot water tower on bubble movement[J]. CIESC Journal, 2019, 70(1): 39-48
胡晨辉, 王亦飞, 包泽彬, 于广锁. 蒸发热水塔内固体颗粒对气泡运动的影响[J]. 化工学报, 2019, 70(1): 39-48 DOI： 10.11949/j.issn.0438-1157.20180697.

HU Chenhui, WANG Yifei, BAO Zebin, YU Guangsuo. Effect of solid particles in evaporative hot water tower on bubble movement[J]. CIESC Journal, 2019, 70(1): 39-48 DOI： 10.11949/j.issn.0438-1157.20180697.

摘要

以蒸发热水塔为研究对象进行可视化实验，借助高速摄像机以及图像处理软件研究热水塔内单孔筛孔塔板上方单个气泡的运动周期及运动特性，孔径为3 mm，在蒸汽中加入不凝性气体N

和N

/固体颗粒的混合物，研究固体颗粒对气泡生成、破碎与过程的影响。实验结果表明：气泡整个生长周期包括生成区、上升区、破碎区。气泡长径比在生成区由大变小，在上升区先增大后减小，在破碎区增大趋势明显；气泡的等效半径在整个运动周期中一直增大，其中在生成区的增大速度最快；生成区气泡的

向运动速率呈现增大趋势，上升区以及破碎区气泡的上升速率平稳波动。当N

带入煤粉颗粒后，发现气泡的上升区时间比例大大降低，破碎区的占比增加明显，有利于塔内的热质传递。

Abstract

The evaporative hot water tower was used as the research object for visualization experiments. The high-speed camera and image processing software were used to study the motion period and characteristics of a single bubble above the single-hole sieve tray in the hot water tower. The aperture was 3 mm. In the experiment process

non-condensable properties were added to the steam. A mixture of gaseous N

and N

/solid particles was used to study the effect of solid particles on bubble formation

fragmentation and processes. The results show that the entire growth cycle of the bubble includes the formation zone

the rising zone and the crushing zone. The ratio of the bubble length to diameter decreases from large to small in the formation zone

increases first and then decreases in the rising zone

and increases in the crushing zone. The equivalent radius of the bubble increases throughout the entire cycle of motion

with the highest growth rate in the formation zone. The

-movement rate of bubbles in the formation zone shows an increasing trend

and the rising rate of bubbles in the rising zone and the crushing zone fluctuates smoothly. When N

was introduced into the pulverized coal particles

it was found that the proportion of the rise time of the bubbles was greatly reduced

and the proportion of the crushing zone increased significantly

which was conducive to the transfer of heat within the tower.

关键词

Keywords

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