论文标题

部分可观测时空混沌系统的无模型预测

Drop encapsulation and bubble bursting in surfactant-laden flows in capillary channels

论文作者

Pico, Paula, Kahouadji, Lyes, Shin, Seungwon, Chergui, Jalel, Juric, Damir, Matar, Omar K.

论文摘要

我们提出了一项参数研究,该研究与在高韦伯数条件下经过液体填充的方形毛细血管的细长气泡流动相关的不稳定现象。这些条件始终诱导在气泡后部形成的重入射流,这通常使液体腔取代。随后的步骤包括腔体中的捏合事件,以生成一个或多个封装的液滴,这些滴剂可能与腔或液滴结合使用气泡 - 液体界面的爆发。这些界面不稳定性中的一些先前已经通过实验报告(Olbricht 1996),并在数值(Izbassarov&Muradoglu 2016)中进行了微液体流量。我们基于混合界面跟踪/水平集方法进行三维直接数值模拟,能够考虑液体散装相和液态气体界面之间的表面活性剂的存在和动态交换。我们的结果表明,惯性,毛细血管,粘度,表面活性剂吸附/解吸动力学和Marangoni应力之间的微妙相互作用对包裹的滴落液泡泡的非轴对称形态结构具有巨大的影响。这种强的耦合还会影响捏合时间,腔体的穿透深度以及整个气泡上包裹的滴剂的数量,大小和速度。根据表面活性剂相关的参数和无量纲组,在三个主要的形态学方面总结了观察到的现象。还提供了有关流程图的讨论。

We present a parametric study of the unsteady phenomena associated with the flow of elongated gas bubbles travelling through liquid-filled square capillaries under high Weber number conditions. These conditions consistently induce the formation of a re-entrant jet at the back of the bubble that commonly gives way to a deep liquid cavity. Subsequent steps include pinch-off events in the cavity to generate one or multiple encapsulated drops which may coalesce, in conjunction with the bursting of the bubble-liquid interface by either the cavity or the drops. Some of these interfacial instabilities have previously been reported experimentally (Olbricht 1996) and numerically (Izbassarov & Muradoglu 2016) for liquid-liquid flow in microchannels. We carry out three-dimensional direct numerical simulations based on a hybrid interface-tracking/level-set method capable of accounting for the presence and dynamic exchange of surfactants between the liquid bulk phase and the liquid-gas interface. Our results indicate that the delicate interplay amongst inertia, capillarity, viscosity, surfactant adsorption/desorption kinetics, and Marangoni stresses has a dramatic influence over the non-axisymmetric morphological structures of the encapsulated drops-elongated bubble. This strong coupling also influences the pinch-off time, penetration depth of the cavity, and number, size, and velocity of the encapsulated drops across the bubble. The observed phenomena are summarised in three main morphological regimes based on surfactant-related parameters and dimensionless groups. A discussion of the flow regime maps is also provided.

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