The motion of a bubble in a non-uniform Hele-Shaw flow

We consider the propagation of a bubble in a non-uniform Hele-Shaw flow. We focus on a distinguished limit in which the bubble is approximately circular in plan view and its velocity is determined by a net force balance incorporating the Hele-Shaw viscous pressure and drag due to the thin films separating the bubble from the cell walls. We find that the instantaneous bubble velocity is the same as that for a bubble in a uniform flow given by the background fluid velocity evaluated at the bubble centre. We apply the model to common microfluidic components, such as a T-junction and injection sources and sinks. Using the same methodology, we derive approximate solutions for the motion of a bubble in more complicated domains including walls or obstacles. We validate the approximate approach with two test cases in which we can find the full solution analytically. First, we consider the effect of an impermeable wall on a bubble in a stagnation-point flow. Second, we consider the motion of a bubble around a circular obstacle. In both cases, the bubble deviates notably from the streamlines of the background flow only when it is very close to the wall or the obstacle.

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Publication Details

Journal
Proceedings of the Royal Society A Mathematical Physical and Engineering Sciences
Published
2025-04-01
DOI
https://doi.org/10.1098/rspa.2024.0613
Citations
2
Primary Topic
Innovative Microfluidic and Catalytic Techniques Innovation
Type
article
Field-Weighted Citation Impact
1.35

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article

The motion of a bubble in a non-uniform Hele-Shaw flow

P. D. Howell, D. J. Booth, Ian M. Griffiths
2 citations
Proceedings of the Royal Society A Mathematical Physical and Engineering Sciences
Innovative Microfluidic and Catalytic Techniques Innovation
1.35
article

The motion of a bubble in a non-uniform Hele-Shaw flow

P. D. Howell, D. J. Booth, Ian M. Griffiths
article en
2 citations

Abstract

We consider the propagation of a bubble in a non-uniform Hele-Shaw flow. We focus on a distinguished limit in which the bubble is approximately circular in plan view and its velocity is determined by a net force balance incorporating the Hele-Shaw viscous pressure and drag due to the thin films separating the bubble from the cell walls. We find that the instantaneous bubble velocity is the same as that for a bubble in a uniform flow given by the background fluid velocity evaluated at the bubble centre. We apply the model to common microfluidic components, such as a T-junction and injection sources and sinks. Using the same methodology, we derive approximate solutions for the motion of a bubble in more complicated domains including walls or obstacles. We validate the approximate approach with two test cases in which we can find the full solution analytically. First, we consider the effect of an impermeable wall on a bubble in a stagnation-point flow. Second, we consider the motion of a bubble around a circular obstacle. In both cases, the bubble deviates notably from the streamlines of the background flow only when it is very close to the wall or the obstacle.

Proceedings of the Royal Society A Mathematical Physical and Engineering SciencesVol. 481(2311)
University of Oxford (GB)
Engineering and Physical Sciences Research Council
Openalex Percentile: Top 21%
Innovative Microfluidic and Catalytic Techniques Innovation
1.35
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The motion of a bubble in a non-uniform Hele-Shaw flow — P. D. Howell, D. J. Booth, et al. · Proceedings of the Royal Society A Mathematical Physical and Engineering Sciences (2025) | TGRS Research Map | TGRS