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应用于通道中二维气泡运动和拓扑变换的粘性泡沫模型:三气泡情况

Viscous froth model applied to the motion and topological transformations of two-dimensional bubbles in a channel: three-bubble case.

作者信息

Torres-Ulloa C, Grassia P

机构信息

Department of Chemical and Process Engineering, University of Strathclyde, James Weir Building, 75 Montrose St, Glasgow G1 1XJ, UK.

出版信息

Proc Math Phys Eng Sci. 2022 Feb;478(2258):20210642. doi: 10.1098/rspa.2021.0642. Epub 2022 Feb 9.

DOI:10.1098/rspa.2021.0642
PMID:35173520
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8826366/
Abstract

The viscous froth model is used to predict rheological behaviour of a two-dimensional (2D) liquid-foam system. The model incorporates three physical phenomena: the viscous drag force, the pressure difference across foam films and the surface tension acting along them with curvature. In the so-called infinite staircase structure, the system does not undergo topological bubble neighbour-exchange transformations for any imposed driving back pressure. Bubbles then flow out of the channel of transport in the same order in which they entered it. By contrast, in a simple single bubble staircase or so-called lens system, topological transformations do occur for high enough imposed back pressures. The three-bubble case interpolates between the infinite staircase and simple staircase/lens. To determine at which driving pressures and at which velocities topological transformations might occur, and how the bubble areas influence their occurrence, steady-state propagating three-bubble solutions are obtained for a range of bubble sizes and imposed back pressures. As an imposed back pressure increases quasi-statically from equilibrium, complex dynamics are exhibited as the systems undergo either topological transformations, reach saddle-node bifurcation points, or asymptote to a geometrically invariant structure which ceases to change as the back pressure is further increased.

摘要

粘性泡沫模型用于预测二维(2D)液体-泡沫系统的流变行为。该模型包含三种物理现象:粘性阻力、泡沫膜两侧的压力差以及沿具有曲率的泡沫膜作用的表面张力。在所谓的无限阶梯结构中,对于任何施加的反向驱动压力,系统都不会发生拓扑气泡邻域交换变换。气泡随后以与进入传输通道相同的顺序流出该通道。相比之下,在简单的单气泡阶梯或所谓的透镜系统中,对于足够高的施加反向压力,确实会发生拓扑变换。三气泡情况介于无限阶梯和简单阶梯/透镜之间。为了确定在哪些驱动压力和速度下可能发生拓扑变换,以及气泡面积如何影响其发生情况,针对一系列气泡尺寸和施加的反向压力,获得了稳态传播三气泡解。当施加的反向压力从平衡状态准静态增加时,随着系统经历拓扑变换、达到鞍结分岔点或渐近到几何不变结构(随着反向压力进一步增加该结构不再变化),会表现出复杂的动力学。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a1e3/8826366/ff6730404b8b/rspa20210642f10.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a1e3/8826366/0b6c5e81afea/rspa20210642f07.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a1e3/8826366/ec9c92e8c672/rspa20210642f08.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a1e3/8826366/ff6730404b8b/rspa20210642f10.jpg

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