Time dependence of effective slip on textured hydrophobic surfaces

• Published in: Physics of fluids (1994) Vol. 21; no. 5; pp. 052001 - 052001-8
• Main Authors: Govardhan, R. N., Srinivas, G. S., Asthana, A., Bobji, M. S.
• Format: Journal Article
• Language: English
• Published: Melville, NY American Institute of Physics 01.05.2009
• Subjects: Condensed matter: structure, mechanical and thermal properties; Exact sciences and technology; Flows in ducts, channels, nozzles, and conduits; Fluid dynamics; Fundamental areas of phenomenology (including applications); Physics; Solid-fluid interfaces; Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties); Wetting; Pipe flow; Wetting; Pressure drop; Microchannel; Slip; Hydrophobicity; Experimental study; Microstructure
• ISSN: 1070-6631; 1089-7666
• DOI: 10.1063/1.3127123

In this paper, we present results on water flow past randomly textured hydrophobic surfaces with relatively large surface features of the order of 50   μ m . Direct shear stress measurements are made on these surfaces in a channel configuration. The measurements indicate that the flow rates required to maintain a shear stress value vary substantially with water immersion time. At small times after filling the channel with water, the flow rates are up to 30% higher compared with the reference hydrophilic surface. With time, the flow rate gradually decreases and in a few hours reaches a value that is nearly the same as the hydrophilic case. Calculations of the effective slip lengths indicate that it varies from about 50   μ m at small times to nearly zero or "no slip" after a few hours. Large effective slip lengths on such hydrophobic surfaces are known to be caused by trapped air pockets in the crevices of the surface. In order to understand the time dependent effective slip length, direct visualization of trapped air pockets is made in stationary water using the principle of total internal reflection of light at the water-air interface of the air pockets. These visualizations indicate that the number of bright spots corresponding to the air pockets decreases with time. This type of gradual disappearance of the trapped air pockets is possibly the reason for the decrease in effective slip length with time in the flow experiments. From the practical point of usage of such surfaces to reduce pressure drop, say, in microchannels, this time scale of the order of 1 h for the reduction in slip length would be very crucial. It would ultimately decide the time over which the surface can usefully provide pressure drop reductions.