Making a splash with water repellency

From Soft-Matter
Revision as of 05:13, 28 September 2009 by Datta (Talk | contribs) (Key Points)

Jump to: navigation, search

Original entry: Sujit S. Datta, APPHY 225, Fall 2009.

Reference

C. Duez, C. Ybert, C. Clanet, and L. Bocquet, Nature Physics 3, 180 (2007).

Keywords

wetting, contact angle, splashing, superhydrophobic

Key Points

What determines how strongly a solid body rushing into a liquid will splash? (For example, consider a sphere being dropped into water). This splash occurs when a pocket of air gets trapped in the fluid after the sphere rushes in, and intuitively, one imagines (correctly) that inertia plays a key role. The purpose of this work was to demonstrate that the surface wettability of the 'intruding' sphere also plays a fundamental role.

This is illustrated by a simple experiment: Duez and co-workers took two identical glass beads, coated one with a very thin layer of silane chains (to make it hydrophobic), and oxidized the other one in a strong etchant (to make it hydrophilic). When both were dropped in the same manner, the hydrophobic one made a larger splash, both visually and in the amplitude of the resulting sound. Furthermore, splashing only occurred for sufficiently large impact velocities - this "threshold" velocity in turn was observed to depend on the surface wettability of the sphere (it was larger for spheres that were more easily wet by the liquid), as well as a characteristic capillary velocity given by <math>\gamma/\mu</math>, where <math>\mu</math> is the viscosity of the liquid.

But why does surface wettability matter? After all, these experiments are done in a regime where inertia dominates over any capillary effects (that is, the Weber number <math>\rho U^2 a/\gamma</math> is large, where <math>\rho</math> is fluid density, <math>U</math> and <math>a</math> are the sphere velocity and size, and <math>\gamma</math> is the fluid surface tension). The answer, of course, lies in exactly how an air pocket is formed after the sphere falls into the water. A clear schematic is shown in figure 3c of the paper: when a sphere falls in, a thin liquid film is formed around it, "climbing" up its body as it continues to fall into the water. The extent to which this film "hugs" the sphere should in some way depend on how well the liquid wets the surface of the sphere: if the