Rheology of two-dimensional dilute emulsions
Phys. Rev. Fluids 11, 033607 – Published 16 March, 2026
DOI: https://doi.org/10.1103/9dgt-rkp5
Abstract
The single droplet under shear is a foundational problem in fluid mechanics. In computational fluid dynamics (CFD), the two-dimensional (2D) problem offers advantages in both computational efficiency and relevance, yet it lacks a comprehensive theoretical treatment equivalent to that of the three-dimensional (3D) case. In this brief note, we present an analytical treatment of this problem beginning with a derivation of the Lamb solution for 2D Stokes flows and then applying it to obtain the flow field around a droplet in a purely extensional flow. Using these flow fields, expressions are obtained for the apparent viscosity, , of a dilute 2D emulsion as well as a small deformation theory. We show that in the limit of both zero Reynolds number () in which inertia is negligible and zero capillary number () in which surface tension prevents any droplet deformations, with where is the ratio of the droplet viscosity to the matrix viscosity and is the area fraction covered by the suspended phase. In addition, we show that in the capillarity-dominated regime (), the steady-state value, , of the Taylor deformation parameter obeys , where Ca is the capillary number and . This contrasts with the 3D case, where depends on . These results are then validated through direct numerical simulations (DNSs) of a single droplet at the center of a periodic square box undergoing simple shear. The DNS and theory are compared across a wide range of viscosity ratios () and area fractions () and they are found to agree asymptotically in the limit for . Our results provide a basic theoretical framework for interpreting 2D droplet simulations and provide clear benchmarks for CFD codes in 2D.