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

机译:淹没孔内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:从浸没孔形成气泡被广泛应用于生物过程和化学反应系统中。在这项研究中,在2D轴对称域上系统地研究了在I期和II期方案中不同孔直径和接触角的影响。模拟结果由第一个气泡的形成给出,并通过周围的流体场,气泡相互作用和气泡长宽比进行解释。孔口直径从0.6 mm到3mm不等。数值结果表明,对于较小的孔直径(d(a)<= 1.5 mm),所有气泡的分离时间均保持恒定(时间),而对于较大的孔,第一个气泡的分离时间与其余气泡的分离时间不同孔直径(d(a)> = 2 mm),这是由于周围流场不同所致。对于气泡配对状态中的气体流速,考虑从60度到165度的接触角,并且观察到,当接触角增大时,气泡脱离时间减小,而当接触角增大时,气泡脱离时间收敛到恒定值。大于135度。此外,观察到了从周期加倍到确定性混乱(每个周期内气泡数量可变)的过渡,并考虑了将浸没管向上插入液体的新方案并将其与以前的情况进行比较。可以看出,当管子垂直插入液体中时,由于周围液体场的影响较大,气泡的脱离时间甚至更短,从而导致了与未插入管子的情况不同的现象。 (C)2019 Elsevier Inc.保留所有权利。

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