Effect of surfactant on elongated bubbles in capillary tubes at high Reynolds number

TL;DR

This study uses 3D numerical simulations to analyze how surfactants influence the dynamics of elongated bubbles in capillary tubes at high Reynolds numbers, revealing surfactant-induced suppression of tail undulations and bubble rigidification.

Contribution

It systematically investigates the effects of various surfactant properties on bubble behavior in inertial flow regimes using advanced numerical methods.

Findings

Surfactants suppress tail undulations by accumulating near the bubble tail.

Large Marangoni stresses cause local bubble rigidification.

Short bubbles can become completely rigid under certain surfactant conditions.

Abstract

The effect of surfactants on the tail and film dynamics of elongated gas bubbles propagating through circular capillary tubes is investigated by means of an extensive three-dimensional numerical study using a hybrid front-tracking/level-set method. The focus is on the visco-inertial regime, which occurs when the Reynolds number of the flow is much larger than unity. Under these conditions, `clean' bubbles exhibit interface undulations in the proximity of the tail \cite{Magnini_prf_2017}, with an amplitude that increases with the Reynolds number. We perform a systematic analysis of the impact of a wide range of surfactant properties, including elasticity, bulk surfactant concentration, solubility, and diffusivity, on the bubble and flow dynamics in the presence of inertial effects. The results show that the introduction of surfactants is effective in suppressing the tail undulations as they tend to accumulate near the bubble tail. Here, large Marangoni stresses are generated, which lead to a local `rigidification' of the bubble. This effect becomes more pronounced for larger surfactant elasticities and adsorption depths. At reduced surfactant solubility, a thicker rigid film region forms at the bubble rear, where a Couette film flow is established, while undulations still appear at the trailing edge of the downstream `clean' film region. In such conditions, the bubble length becomes an influential parameter, with short bubbles becoming completely rigid.