Coutinho Írio M, Anjos Pedro H A, Oliveira Rafael M, Miranda José A
Departamento de Física, Universidade Federal de Pernambuco, CCEN, Recife, Pernambuco 50670-901, Brazil.
Departamento de Engenharia Mecânica, Pontifícia Universidade Católica do Rio de Janeiro, Rio de Janeiro 22451-900, Brazil.
Phys Rev E. 2024 Jan;109(1-2):015104. doi: 10.1103/PhysRevE.109.015104.
The lifting Hele-Shaw cell flow commonly involves the stretching of a viscous oil droplet surrounded by air, in the confined space between two parallel plates. As the upper plate is lifted, viscous fingering instabilities emerge at the air-oil interface. Such an interfacial instability phenomenon is widely observed in numerous technological and industrial applications, being quite difficult to control. Motivated by the recent interest in controlling and stabilizing the Saffman-Taylor instability in lifting Hele-Shaw flows, we propose an alternative way to restrain the development of interfacial disturbances in this gap-variable system. Our method modifies the traditional plate-lifting flow arrangement by introducing a finite fluid annulus layer encircling the central oil droplet, and separating it from the air. A second-order, perturbative mode-coupling approach is employed to analyze morphological and stability behaviors in this three-fluid, two-interface, doubly connected system. Our findings indicate that the intermediate fluid ring can significantly stabilize the interface of the central oil droplet. We show that the effectiveness of this stabilization protocol relies on the appropriate choice of the ring's viscosity and thickness. Furthermore, we calculate the adhesion force required to detach the plates, and find that it does not change significantly with the addition of the fluid envelope as long as it is sufficiently thin. Finally, we detect no distinction in the adhesion force computed for stable or unstable annular interfaces, indicating that the presence of fingering at the ring's boundaries has a negligible effect on the adhesion force.
提升型赫勒-肖细胞流通常涉及在两个平行板之间的狭窄空间中,一个被空气包围的粘性油滴的拉伸。当上板被抬起时,在空气-油界面处会出现粘性指进不稳定性。这种界面不稳定性现象在众多技术和工业应用中广泛存在,很难控制。受近期对控制和稳定提升型赫勒-肖流中萨夫曼-泰勒不稳定性的关注的启发,我们提出了一种在这个间隙可变系统中抑制界面扰动发展的替代方法。我们的方法通过引入一个围绕中心油滴的有限流体环形层,并将其与空气隔开,对传统的板提升流布置进行了修改。采用二阶微扰模式耦合方法来分析这个三流体、双界面、双连通系统中的形态和稳定性行为。我们的研究结果表明,中间流体环可以显著稳定中心油滴的界面。我们表明,这种稳定方案的有效性依赖于对环的粘度和厚度的适当选择。此外,我们计算了分离板所需的粘附力,发现只要流体包层足够薄,添加流体包层后粘附力不会有显著变化。最后,我们发现在计算稳定或不稳定环形界面的粘附力时没有区别,这表明环边界处的指进现象对粘附力的影响可以忽略不计。