Using
atomic force microscopy, the nanofriction coefficient was
measured systematically for a series of liquids on planar graphite,
silica and mica surfaces. This allows us to explore the quantitative
interplay between nanofriction at liquid–solid interfaces and
interfacial wetting. A corresponding states theory analysis shows
that the nanofriction coefficient, μ = d<i>F</i><sub>F</sub>/d<i>F</i><sub>N</sub>, where <i>F</i><sub>F</sub> is the friction force and <i>F</i><sub>N</sub> is the normal force, is a function of three dimensionless parameters
that reflect the intermolecular forces involved and the structure
of the solid substrate. Of these, we show that one parameter in particular,
β = ρ<sub>s</sub>Δ<sub>s</sub>σ<sub>ls</sub><sup>2</sup>, where ρ<sub>s</sub> is the atomic density of
the solid, Δ<sub>s</sub> is the spacing between layers of solid
atoms, and σ<sub>ls</sub> is the molecular diameter that characterizes
the liquid–substrate interaction, is very important in determining
the friction coefficient. This parameter β, which we term the <i>structure adhesion parameter</i>, provides a measure of the
intermolecular interaction between a liquid molecule and the substrate
and also of the surface area of contact of the liquid molecule with
the substrate. We find a linear dependence of μ on the structure
adhesion parameter for the systems studied. We also find that increasing
β leads to an increase in the vertical adhesion forces <i>F</i><sub>A</sub> (the attractive force exerted by the solid
surface on the liquid film). Our quantitative relationship between
the nanofriction coefficient and the key parameter β which governs
the vertical adhesive strength, opens up an opportunity for describing
liquid flows on solid surfaces at the molecular level, with implications
for the development of membrane and nanofluidic devices
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