改进一次油分离中气泡-液滴相互作用的实验研究

Joel R. Karp, E. Mancilla, P. H. Santos, M. M. Neto, R. Morales
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引用次数: 0

摘要

实验研究了分散的油滴与气泡之间的相互作用。在帕拉南联邦理工大学(UTFPR)多相流研究中心(NUEM)建立了一个实验装置,利用侧视图流动可视化技术对固相气泡和油滴之间的相互作用进行了基本评估。以自来水为连续相,以纯氮和有色植物油为分散相。气泡-液滴附着是指气泡被液滴包裹,在现象学上与液滴-液滴聚结相似。分散相之间的接触形成了一个连接桥,随着时间的推移,桥的高度迅速增长,在57.0 ms后,桥的高度与液滴的大小相当。这种现象固有的不对称性导致气泡向液滴的显著水平位移,液滴的位置保持不变。桥半月板的评估证实了这一观察,因为液滴侧的接触角比气泡侧的接触角随时间衰减得更快。通过获得上升集料的大小、三维轨迹和最终速度,对上升集料的流体力学进行了评价。基于单个液滴的终端速度,形成的稳定团聚体增加了150 ~ 180%。研究发现,气泡半径是影响聚集体流体动力学的主要因素,因此可以根据轨迹不稳定性定义临界气泡半径。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Experimental Study of Bubble-Droplet Interactions in Improved Primary Oil Separation
The interactions between dispersed oil droplets and gas bubbles was experimentally studied in this work. An experimental set-up was built in the Multiphase Flow Research Center (NUEM) in the Federal University of Technology – Paraná (UTFPR) to conduct a fundamental evaluation of the interactions between sessile gas bubbles and oil droplets employing side-view flow visualization. Tap water was used as the continuous phase, whereas pure nitrogen and colored vegetable oil were employed as the dispersed phases. The bubble-droplet attachment consisted in the encapsulation of the bubble by the droplet, presenting phenomenological similarities to droplet-droplet coalescence. The contact between the dispersed phases induces the formation of a connecting bridge, which grows rapidly with time, with the height of the bridge being comparable to the size of the droplet after 57.0 ms. The inherent asymmetry of the phenomenon induced a significant horizontal displacement of the bubble towards the droplet, whose position remained unaltered. The evaluation of the bridge meniscus corroborated to this observation, since the contact angle on the droplet side decayed faster with time in comparison to the contact angle on the bubble side. The hydrodynamics of the rising aggregate is also evaluated, by the obtainment of its size, three-dimensional trajectory and terminal velocity. The stable aggregates formed presented an increase factor of 150 to 180%, based on the terminal velocity of the individual droplet. The radius of the bubble was found to be the major influence on the hydrodynamics of the aggregate, allowing the definition of a critical bubble radius based on trajectory instabilities.
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