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A small vicinity of a contact line, with well-defined (micro)scales (henceforth the
“microstructure”), is studied theoretically for a system of a perfectly wetting liquid,
its pure vapor and a superheated flat substrate. At one end, the microstructure terminates
in a non-evaporating microfilm owing to the disjoining-pressure-induced Kelvin effect. At
the other end, for motionless contact lines, it terminates in a constant film slope
(apparent contact...
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