An Experimental Procedure to Obtain the Equilibrium Contact Angle from the Wilhelmy Method

The theory of contact angles has been developed using the concept of the Young contact angle, an equilibrium quantity related to perfectly smooth and homogeneous surfaces; on real surfaces it is commonly accepted that one can obtain metastableequilibrium states, in which the shape of the meniscus along the triple line is not fully equivalent to the equilibriummeniscus. In the present paper, a new method is presented to obtain an equilibrium contact angle with a simple modification of the Wilhelmy microbalance. The supply of acoustic energy to the liquid at a frequency which induces the resonant formation of capillary waves, followed by the reduction of the amplitude of the vibration, allows the meniscus to move from the metastable advancing or receding shape to the stable equilibrium one. This result appears to be significantly independent of the initial conditions; it has been possible to confirm the theoretical provision that the energy barriers between metastable states far from equilibrium are lower than the barriers at equilibrium. The equation which relates the equilibrium cosine of the contact angle and the mean of advancing and receding cosines has been confirmed on homogeneous surfaces, but has been disproved on macroscopically heterogeneous surfaces. The method appears promising also for its simplicity and low cost.

[1]  T. Young III. An essay on the cohesion of fluids , 1805, Philosophical Transactions of the Royal Society of London.

[2]  R. N. Wenzel RESISTANCE OF SOLID SURFACES TO WETTING BY WATER , 1936 .

[3]  F. Fowkes,et al.  The State of Monolayers Adsorbed at the Interface Solid—Aqueous Solution , 1940 .

[4]  A. Cassie,et al.  Wettability of porous surfaces , 1944 .

[5]  R. Shuttleworth,et al.  The spreading of a liquid over a rough solid , 1948 .

[6]  R. H. Dettre,et al.  Contact Angle Hysteresis. III. Study of an Idealized Heterogeneous Surface , 1964 .

[7]  J. Lane,et al.  A thermodynamic discussion of the use of a vertical-plate balance for the measurement of surface tension , 1964 .

[8]  R. Good,et al.  Thermodynamics of contact angles. I. Heterogeneous solid surfaces , 1972 .

[9]  Terence Desmond Blake,et al.  Contact-Angle Hysteresis , 1973 .

[10]  A. Neumann,et al.  Thermodynamics of contact angles. II. Rough solid surfaces , 1975 .

[11]  Chun Huh,et al.  Effects of surface roughness on wetting (theoretical) , 1977 .

[12]  Tennyson Smith,et al.  Effect of acoustic energy on contact angle measurements , 1978 .

[13]  P. G. de Gennes,et al.  A model for contact angle hysteresis , 1984 .

[14]  K. Birdi,et al.  Wettability and Contact Angles , 1984 .

[15]  Joseph D. Andrade,et al.  The Contact Angle and Interface Energetics , 1985 .

[16]  W. Possart,et al.  Young's equilibrium contact angle on rough solid surfaces. Part I. An empirical determination , 1989 .

[17]  Victor Starov,et al.  EQUILIBRIUM AND HYSTERESIS CONTACT ANGLES , 1992 .

[18]  J.-M. di Meglio Contact Angle Hysteresis and Interacting Surface Defects , 1992 .

[19]  C. Sykes,et al.  Average spreading parameter on heterogeneous surfaces , 1994 .

[20]  Dongqing Li,et al.  THERMODYNAMIC STATUS OF CONTACT ANGLES , 1996 .

[21]  S. Garoff,et al.  Using Vibrational Noise To Probe Energy Barriers Producing Contact Angle Hysteresis , 1996 .

[22]  C. Volpe,et al.  Some Reflections on Acid-Base Solid Surface Free Energy Theories , 1997, Journal of colloid and interface science.

[23]  R. M. Cannon,et al.  Ridging effects on wetting and spreading of liquids on solids , 1998 .

[24]  S. Garoff,et al.  Physics of contact angle measurement , 1999 .

[25]  Öpik Contact-Angle Hysteresis Caused by a Random Distribution of Weak Heterogeneities on a Solid Surface. , 2000, Journal of colloid and interface science.

[26]  S. Siboni,et al.  Acid–base surface free energies of solids and the definition of scales in the Good–van Oss–Chaudhury theory , 2000 .