Shear induced breakup of droplets in a colloidal dispersion

TL;DR

This study uses numerical simulations to analyze how shear flow causes droplets in colloidal dispersions to break up, revealing the dependence on a velocity ratio and confirming a theoretical hypothesis.

Contribution

The paper introduces a numerical approach to study droplet breakup in colloidal dispersions, confirming the velocity ratio's role and extending understanding of breakup conditions.

Findings

Critical capillary number depends on velocity ratio E.

For E<10, breakup behavior aligns with Taylor's regime.

For E>10, Ca_B behaves as 2/E, confirming previous hypothesis.

Abstract

We present numerical results for the breakup of a pair of colloidal particles enveloped by a droplet under shear flow. The smoothed profile method is used to accurately account for the hydrodynamic interactions between particles due to the host fluid. We observe that the critical capillary number, $Ca_{\rm B}$, at which droplets breakup depends on a velocity ratio, $E$, defined as the ratio of the boundary shift velocity (that restores the droplet shape to a sphere) to the diffusive flux velocity in units of the particle radius $a$. For $E < 10$, $Ca_{B}$ is independent of $E$, as is consistent with the regime studied by Taylor. When $E > 10$, $Ca_{B}$ behaves as $Ca_{\rm B} = 2E^{-1}$, which confirms Karam and Bellinger's hypothesis. As a consequence, droplet break up will occur when the time scale of droplet deformation $\dot{\gamma}^{-1}$ is smaller than the diffusive time scale $t_{D} \equiv a^{2}/L\tau$ in units of $a$, where $L$ is the diffusion constant and $\tau$ is the 2nd order coefficient of the Ginzburg-Landau type free energy of the binary mixture. We emphasize that the breakup of droplet dispersed particles is not only governed by a balance of forces. We find that velocity competition is one of the important contributing factor.