TY - JOUR
T1 - To wet or not to wet
T2 - That is the question
AU - Gatica, Silvina M.
AU - Cole, Milton W.
N1 - Funding Information:
Acknowledgements We would like to both acknowledge support of this research by NSF and thank the following colleagues and collaborators for many helpful discussions, as well as assistance with figures: Francesco Ancilotto, Mary J. Bojan, Massimo Boninsegni, Carlo Carraro, Moses Chan, Andrew Chizmeshya, Stefano Curtarolo, Renee Diehl, Rafael Garcia, Susana Hernández, George Hess, Karl Johnson, Kevin Lehmann, Hye-Young Kim, Scott Milner, Mike Pettersen, Will Saam, George Stan, Bill Steele, Peter Taborek, Flavio Toigo, Gianfranco Vidali, Makoto Yao and Xiongce Zhao.
PY - 2009
Y1 - 2009
N2 - Wetting transitions have been predicted and observed to occur for various combinations of fluids and surfaces. This paper describes the origin of such transitions, for liquid films on solid surfaces, in terms of the gas-surface interaction potentials V(r), which d epend on the specific adsorption system. The transitions of light inert gases and H 2 molecules on alkali metal surfaces have been explored extensively and are relatively well understood in terms of the least attractive adsorption interactions in nature. Much less thoroughly investigated are wetting transitions of Hg, H 2O, heavy inert gases and other molecular films. The basic idea is that nonwetting occurs, for energetic reasons, if the adsorption potential's well-depth D is smaller than, or comparable to, the well-depth ε of the adsorbate-adsorbate mutual interaction. At the wetting temperature, T w, the transition to wetting occurs, for entropic reasons, when the liquid's surface tension is sufficiently small that the free energy cost in forming a thick film is sufficiently compensated by the fluid-surface interaction energy. Guidelines useful for exploring wetting transitions of other systems are analyzed, in terms of generic criteria involving the "simple model", which yields results in terms of gas-surface interaction parameters and thermodynamic properties of the bulk adsorbate.
AB - Wetting transitions have been predicted and observed to occur for various combinations of fluids and surfaces. This paper describes the origin of such transitions, for liquid films on solid surfaces, in terms of the gas-surface interaction potentials V(r), which d epend on the specific adsorption system. The transitions of light inert gases and H 2 molecules on alkali metal surfaces have been explored extensively and are relatively well understood in terms of the least attractive adsorption interactions in nature. Much less thoroughly investigated are wetting transitions of Hg, H 2O, heavy inert gases and other molecular films. The basic idea is that nonwetting occurs, for energetic reasons, if the adsorption potential's well-depth D is smaller than, or comparable to, the well-depth ε of the adsorbate-adsorbate mutual interaction. At the wetting temperature, T w, the transition to wetting occurs, for entropic reasons, when the liquid's surface tension is sufficiently small that the free energy cost in forming a thick film is sufficiently compensated by the fluid-surface interaction energy. Guidelines useful for exploring wetting transitions of other systems are analyzed, in terms of generic criteria involving the "simple model", which yields results in terms of gas-surface interaction parameters and thermodynamic properties of the bulk adsorbate.
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U2 - 10.1007/s10909-009-9885-z
DO - 10.1007/s10909-009-9885-z
M3 - Article
AN - SCOPUS:70349662350
SN - 0022-2291
VL - 157
SP - 111
EP - 136
JO - Journal of Low Temperature Physics
JF - Journal of Low Temperature Physics
IS - 3-4
ER -