论文标题

一对可变形气泡的三维动力学最初在线上升高。第1部分:适度惯性制度

Three-dimensional dynamics of a pair of deformable bubbles rising initially in line. Part 1: Moderately inertial regimes

论文作者

Zhang, Jie, Ni, Ming-Jiu, Magnaudet, Jacques

论文摘要

在高度分辨的模拟的帮助下检查了两个相同气泡在静止液体中释放的相同气泡的浮力运动,重点是中等惯性方向,其中隔离气泡的路径是垂直的。假设首先是轴对称的演化,则气泡对的平衡构型是根据浮力对粘合和浮力 - 毛细血管对的函数确定的,该功率分别定义了系统的数量($ GA $)和债券($ bo $)。三维溶液表明,实际上从未达到这种轴对称平衡。取而代之的是,提供$ bo $的含量低于至关重要的$ ga $依赖性阈值,确定了结合的开始,观察到了两个明显不同的演变。在探索的$(GA,\,BO)$ - 范围的下端,串联遵循起草敲击的场景,最终会并肩运动。对于较大的$ ga $,落后的气泡横向漂移,并从领先的泡沫中脱颖而出,几乎不会改变后者的路径。在第二种情况下,晚期配置的特征是串联的倾向从$ 30^\ circ $到$ 40^\ circ $相对于垂直行业。气泡变形对系统的演变有重大影响。它控制着领先气泡后控制涡度效应的大小,因此,引起尾巴上的吸引力的强度。它还控制着作用在这种气泡上的强度甚至迹象,当串联释放出较小的角度偏差时,这种机制特别重要。

The buoyancy-driven motion of two identical gas bubbles released in line in a liquid at rest is examined with the help of highly resolved simulations, focusing on moderately inertial regimes in which the path of an isolated bubble is vertical. Assuming first an axisymmetric evolution, equilibrium configurations of the bubble pair are determined as a function of the buoyancy-to-viscous and buoyancy-to-capillary force ratios which define the Galilei ($Ga$) and Bond ($Bo$) numbers of the system, respectively. The three-dimensional solutions reveal that this axisymmetric equilibrium is actually never reached. Instead, provided $Bo$ stands below a critical $Ga$-dependent threshold determining the onset of coalescence, two markedly different evolutions are observed. At the lower end of the explored $(Ga,\,Bo)$-range, the tandem follows a Drafting-Kissing-Tumbling scenario which eventually yields a planar side-by-side motion. For larger $Ga$, the trailing bubble drifts laterally and gets out of the wake of the leading bubble, barely altering the path of the latter. In this second scenario, the late configuration is characterized by a significant inclination of the tandem ranging from $30^\circ$ to $40^\circ$ with respect to the vertical. Bubble deformation has a major influence on the evolution of the system. It controls the magnitude of vortical effects in the wake of the leading bubble, hence the strength of the attractive force acting on the trailing bubble. It also governs the strength and even the sign of the lateral force acting on this bubble, a mechanism of particular importance when the tandem is released with a small angular deviation.

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