Droplet migration in a Hele-Shaw cell: Effect of the lubrication film on the droplet dynamics

TL;DR

This study uses three-dimensional simulations to analyze how the lubrication film affects droplet movement in a Hele-Shaw cell, revealing that traditional models overlook critical lubrication effects impacting droplet velocity.

Contribution

The paper demonstrates the significant influence of the lubrication film on droplet velocity and flow structure, highlighting limitations of classic Hele-Shaw models in low-migration scenarios.

Findings

Lubrication film reduces droplet velocity compared to inflow velocity.

Droplet shape becomes pancake-like when radius exceeds half the channel height.

Droplet velocity decreases with increasing capillary number.

Abstract

Droplet migration in a Hele--Shaw cell is a fundamental multiphase flow problem which is crucial for many microfluidics applications. We focus on the regime at low capillary number and three-dimensional direct numerical simulations are performed to investigate the problem. In order to reduce the computational cost, an adaptive mesh is employed and high mesh resolution is only used near the interface. Parametric studies are performed on the droplet horizontal radius and the capillary number. For droplets with an horizontal radius larger than half the channel height the droplet overfills the channel and exhibits a pancake shape. A lubrication film is formed between the droplet and the wall and particular attention is paid to the effect of the lubrication film on the droplet velocity. The computed velocity of the pancake droplet is shown to be lower than the average inflow velocity, which is in agreement with experimental measurements. The numerical results show that both the strong shear induced by the lubrication film and the three-dimensional flow structure contribute to the low mobility of the droplet. In this low-migration-velocity scenario the interfacial flow in the droplet reference frame moves toward the rear on the top and reverses direction moving to the front from the two side edges. The velocity of the pancake droplet and the thickness of the lubrication film are observed to decrease with capillary number. The droplet velocity and its dependence on capillary number cannot be captured by the classic Hele--Shaw equations, since the depth-averaged approximation neglects the effect of the lubrication film.