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Numerical study of formation of a series of bubbles at a submerged orifice

机译:淹没孔口一系列气泡形成的数值研究

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Bubble formation from a submerged orifice is widely applied in bio-process and chemical reaction systems. In this study, the effects of different orifice diameters and contact angles in Period-I and Period-II regimes are studied systematically on a 2D axisymmetric domain. Simulation results are presented from the formation of the first bubble and explained by means of the surrounding fluid field, bubble interaction, and bubble aspect ratio.The orifice diameter is varied from 0.6 mm to 3mm. The numerical results show that the detachment time of all bubbles remains constant (in time) for smaller orifice diameters (d(a) = 1.5 mm), while the detachment time of the first bubble is different from the rest of the bubbles for larger orifice diameters (d(a) = 2 mm), which is due to the different surrounding flow field. Contact angles from 60 degrees to 165 degrees are considered for the gas flow rates in the regime of bubble pairing, and it is observed that the bubble detachment time decreases when the contact angle increases, and it converges to a constant value when the contact angle is larger than 135 degrees. In addition, the transition from period doubling to deterministic chaos (in which there is a variable number of bubbles within each period) is observed.A new scenario of inserting a submerged tube upward into the liquid is considered and compared to the previous cases. It is observed that when the tube is vertically inserted into the liquid, the bubble detachment time is even smaller because of higher influence from the surrounding liquid field, leading to a different phenomenon from the non-inserted tube cases. (C) 2019 Elsevier Inc. All rights reserved.
机译:来自浸没孔的气泡形成广泛应用于生物过程和化学反应系统。在该研究中,系统地在2D轴对称结构域上对不同孔径直径和接触角的影响和周期-I型制度的影响。仿真结果由第一气泡的形成提出,并通过周围的流体场,气泡相互作用和气泡纵横比说明。孔口直径从0.6mm到3mm变化。数值结果表明,对于更小的孔径直径(D(a)<= 1.5mm),所有气泡的分离时间保持恒定(及时),而第一气泡的分离时间与较大的剩余气泡的脱离时间不同孔口直径(D(a)> = 2mm),这是由于周围的周围流场不同。在气泡配对的状态下,考虑从60度到165度的接触角,并且观察到当接触角增加时气泡分离时间减小,并且当接触角是时,它会收敛到恒定值大于135度。另外,观察到从周期倍增到确定性混沌(其中每个时段内的可变数量的气泡)的转变。考虑并将向上插入液体中的新场景,并将其与先前的情况相比。观察到,当管垂直插入液体时,由于从周围的液体场的影响较高,气泡脱离时间甚至更小,导致来自未插入的管道壳的不同现象。 (c)2019 Elsevier Inc.保留所有权利。

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