4.7 Article

Physical mechanisms for droplet size and effective viscosity asymmetries in turbulent emulsions

期刊

JOURNAL OF FLUID MECHANICS
卷 951, 期 -, 页码 -

出版社

CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2022.881

关键词

multiphase flow; Taylor-Couette flow; turbulent convection

资金

  1. National Natural Science Foundation of China [11988102, 91852202]
  2. Tencent Foundation through the Xplorer Prize

向作者/读者索取更多资源

This study investigates the microscopic droplet size and macroscopic rheology of emulsions in a Taylor-Couette turbulent shear flow by varying the oil volume fraction. It is found that oil-in-water (O/W) and water-in-oil (W/O) emulsions exhibit distinct hydrodynamic behaviors, which can be attributed to the presence of surface-active contaminants. The addition of an oil-soluble surfactant restores the symmetry between O/W and W/O emulsions. Furthermore, the droplet size in turbulent emulsions is determined by dynamic pressure caused by the gradient of the mean flow rather than turbulent fluctuations.
By varying the oil volume fraction, the microscopic droplet size and the macroscopic rheology of emulsions are investigated in a Taylor-Couette turbulent shear flow. Although here oil and water in the emulsions have almost the same physical properties (density and viscosity), unexpectedly, we find that oil-in-water (O/W) and water-in-oil (W/O) emulsions have very distinct hydrodynamic behaviours, i.e. the system is clearly asymmetric. By looking at the micro-scales, the average droplet diameter hardly changes with the oil volume fraction for O/W or for W/O. However, for W/O it is about 50% larger than that of O/W. At the macro-scales, the effective viscosity of O/W is higher when compared to that of W/O. These asymmetric behaviours are expected to be caused by the presence of surface-active contaminants from the walls of the system. By introducing an oil-soluble surfactant at high concentration, remarkably, we recover the symmetry (droplet size and effective viscosity) between O/W and W/O emulsions. Based on this, we suggest a possible mechanism responsible for the initial asymmetry and reach conclusions on emulsions where interfaces are fully covered by the surfactant. Next, we discuss what sets the droplet size in turbulent emulsions. We uncover a -6/5 scaling dependence of the droplet size on the Reynolds number of the flow. Combining the scaling dependence and the droplet Weber number, we conclude that the droplet fragmentation, which determines the droplet size, occurs within the boundary layer and is controlled by the dynamic pressure caused by the gradient of the mean flow, as proposed by Levich (Physicochemical Hydrodynamics, Prentice-Hall, 1962), instead of the dynamic pressure due to turbulent fluctuations, as proposed by Kolmogorov (Dokl. Akad. Nauk. SSSR, vol. 66, 1949, pp. 825-828). The present findings provide an understanding of both the microscopic droplet formation and the macroscopic rheological behaviours in dynamic emulsification, and connects them.

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