Effects of surface wettability and liquid viscosity on the dynamic wetting of individual drops

被引:97
作者
Chen, Longquan [1 ]
Bonaccurso, Elmar [1 ]
机构
[1] Tech Univ Darmstadt, Ctr Smart Interfaces, D-64287 Darmstadt, Germany
来源
PHYSICAL REVIEW E | 2014年 / 90卷 / 02期
关键词
PRECURSOR; KINETICS; OIL;
D O I
10.1103/PhysRevE.90.022401
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
In this paper, we experimentally investigated the dynamic spreading of liquid drops on solid surfaces. Drop of glycerol water mixtures and pure water that have comparable surface tensions (62.3-72.8 mN/m) but different viscosities (1.0-60.1 cP) were used. The size of the drops was 0.5-1.2 mm. Solid surfaces with different lyophilic and lyophobic coatings (equilibrium contact angle theta(eq) of 0 degrees-112 degrees) were used to study the effect of surface wettability. We show that surface wettability and liquid viscosity influence wetting dynamics and affect either the coefficient or the exponent of the power law that describes the growth of the wetting radius. In the early inertial wetting regime, the coefficient of the wetting power law increases with surface wettability but decreases with liquid viscosity. In contrast, the exponent of the power law does only depend on surface wettability as also reported in literature. It was further found that surface wettability does not affect the duration of inertial wetting, whereas the viscosity of the liquid does. For low viscosity liquids, the duration of inertial wetting corresponds to the time of capillary wave propagation, which can be determined by Lamb's drop oscillation model for inviscid liquids. For relatively high viscosity liquids, the inertial wetting time increases with liquid viscosity, which may due to the viscous damping of the surface capillary waves. Furthermore, we observed a viscous wetting regime only on surfaces with an equilibrium contact angle theta(eq) smaller than a critical angle theta(c) depending on viscosity. A scaling analysis based on Navier-Stokes equations is presented at the end, and the predicted theta(c) matches with experimental observations without any additional fitting parameters.
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页数:9
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