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Controlling droplet bouncing and coalescence with surfactant

Published online by Cambridge University Press:  28 June 2016

K.-L. Pan ,
Y.-H. Tseng ,
J.-C. Chen ,
K.-L. Huang ,
C.-H. Wang  and
M.-C. Lai
K.-L. Pan*
Affiliation:
Department of Mechanical Engineering, National Taiwan University, Taipei 10617, Taiwan, ROC
Y.-H. Tseng
Affiliation:
Department of Applied Mathematics, National University of Kaohsiung, Kaohsiung 81148, Taiwan, ROC
J.-C. Chen
Affiliation:
Department of Mechanical Engineering, National Taiwan University, Taipei 10617, Taiwan, ROC
K.-L. Huang
Affiliation:
Department of Mechanical Engineering, National Taiwan University, Taipei 10617, Taiwan, ROC
C.-H. Wang
Affiliation:
Department of Mechanical Engineering, National Taiwan University, Taipei 10617, Taiwan, ROC
M.-C. Lai
Affiliation:
Department of Applied Mathematics, National Chiao Tung University, Hsinchu 30050, Taiwan, ROC
*
†Email address for correspondence: [email protected]
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Abstract

The collision between aqueous drops in air typically leads to coalescence after impact. Rebounding of the droplets with similar sizes at atmospheric conditions is not generated, unless with significantly large pressure or high impact parameters exhibiting near-grazing collision. Here we demonstrate experimentally the creation of a non-coalescent regime through addition of a small amount of water-soluble surfactant. We perform a direct simulation to account for the continuum and short-range flow dynamics of the approaching interfaces, as affected by the soluble surfactant. Based on the immersed-boundary formulation, a conservative scheme is developed for solving the coupled surface-bulk convection–diffusion concentration equations, which presents excellent mass preservation in the solvent as well as conservation of total surfactant mass. We show that the Marangoni effect, caused by non-uniform distributions of surfactant on the droplet surface and surface tension, induces stresses that oppose the draining of gas in the interstitial gap, and hence prohibits merging of the interfaces. In such gas–liquid systems, the repulsion caused by the addition of surfactant, as frequently observed in liquid–liquid systems such as emulsions in the form of an electric double-layer force, was found to be too weak to dominate in the attainable range of interfacial separation distances. These results thus identify the key mechanisms governing the impact dynamics of surfactant-coated droplets in air and imply the potential of using a small amount of surfactant to manipulate impact outcomes, for example, to prevent coalescence between droplets or interfaces in gases.

JFM classification

Drops and Bubbles: Breakup/coalescence Drops and Bubbles: Drops
Type
Papers
Information
Journal of Fluid Mechanics , Volume 799 , 25 July 2016 , pp. 603 - 636
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Copyright
© 2016 Cambridge University Press 

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