Abstract

An understanding of the dynamics of growth-driven coalescence is important in diverse fields across natural science and engineering. Motivated by the bubble coalescence in magma during volcanic eruptions, we study both experimentally and theoretically the coalescence of two growing bubbles in a Hele–Shaw cell. In our system, bubbles grow by gas expansion due to decompression and the diffusional influx of dissolved gas in the liquid. Our experiments show that the evolution of film thickness and bubble shape depends on viscosity, decompression rate, and cell gap. Through a scaling analysis and a perturbation approximation, we find that the hydrodynamic interaction between two bubbles is characterized by a film capillary number Ca_f=(eta {dot{R}}/sigma )(R/D)^2 depending on viscosity eta, bubble radius R, growth rate {dot{R}}, interfacial tension sigma, and cell gap D. The experimental results demonstrate that the film capillary number solely determines the bubble distortion just before coalescence. Under our experimental conditions, bubble coalescence occurs below a critical value of a nominal film capillary number defined as a film capillary number evaluated when two undeformed circular bubbles come into contact.

Highlights

  • An understanding of the dynamics of growth-driven coalescence is important in diverse fields across natural science and engineering

  • Bubble growth is driven by two mechanisms: gas expansion, which we assume follows behaviour according to the ideal gas law, and the diffusional influx of dissolved air

  • We have considered the condition of bubble coalescence and the bubble shape just before coalescence

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Summary

Introduction

An understanding of the dynamics of growth-driven coalescence is important in diverse fields across natural science and engineering. Most previous studies on bubble coalescence have focused on the film drainage in a low-viscosity liquid by moving a bubble of constant volume to another bubble or free s­ urface[12,13,14] The coalescence in these studies is controlled by inertia force and is different from the growth-driven coalescence in a more viscous liquid, such as magma and polymers. For understanding of foam formation, gas bubbles have to be used because the viscous resistance in a film is sensitive to the boundary condition between the bubble (or drop) and the surrounding liquid Another in-situ experimental design used a quasi-two-dimensional cell in which a bubble suspension is clamped with two transparent plates and separated by a small ­gap[18,19,20,21,22]. The thin cell makes it possible to observe bubble coalescence without

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