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    Rheology of two-dimensional dilute emulsions

    Thomas Appleford1,*, Vatsal Sanjay2, and Maziyar Jalaal1,†

    • *Contact author: t.appleford@uva.nl
    • †Contact author: m.jalaal@uva.nl

    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, μ*, of a dilute 2D emulsion as well as a small deformation theory. We show that in the limit of both zero Reynolds number (Re→0) in which inertia is negligible and zero capillary number (Ca→0) in which surface tension prevents any droplet deformations, μ*=μ(1+f(λ)ϕ)+O(ϕ2) with f(λ)=(2λ+1)/(λ+1) where λ is the ratio of the droplet viscosity to the matrix viscosity and ϕ is the area fraction covered by the suspended phase. In addition, we show that in the capillarity-dominated regime (Ca≪1), the steady-state value, DT∞, of the Taylor deformation parameter obeys DT∞=g(λ)Ca, where Ca is the capillary number and g(λ)=1. This contrasts with the 3D case, where g(λ) depends on λ. 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 (0.01≤λ≤100) and area fractions (0.002≤ϕ≤0.125) and they are found to agree asymptotically in the limit ϕ→0 for Ca≪1/(λ+1). Our results provide a basic theoretical framework for interpreting 2D droplet simulations and provide clear benchmarks for CFD codes in 2D.

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