Hideki Kobayashi, Hiroshi Morita
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 larger 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.
View original:
http://arxiv.org/abs/1211.1297
No comments:
Post a Comment