The spreading parameter S is the fundamental parameter controlling the
stability of thin liquid films intercalated between a hydrophobic sol
id and a soft elastomer (Young modulus E): S = gamma(SR)-(gamma(SL) gamma(LR)), where gamma(SR), gamma(SL), and gamma(LR) are respectively
the solid/elastomer, solid/liquid, and liquid/elastomer interfacial t
ensions. We describe here a simple experimental method to determine S.
We monitor by interferometry the profile of liquid droplets squeezed
at the solid/elastomer interface. S is negative and the droplets do no
t spread. We find that (i) an intercalated droplet is a very flat semi
ellipsoid with a macroscopic contact angle of 90 degrees and (ii) the
radius R of the wet area scales like R proportional to H-2/h(0), where
H is the thickness at the center and h(0) = \S\/E is a characteristic
length in the range of 100 Angstrom. From the shape analysis we extra
ct h(0) and as a consequence the spreading parameter S. This measureme
nt was performed for different liquids sandwiched between a cross-link
ed silicone polymer and chemically modified glass slides. Liquid dropl
ets trapped at the solid/elastomer interface give similar results exce
pt that we get ellipsoid instead of semi-ellipsoid. In this particular
case the spreading parameter is simply given by S = 2 gamma(LR) and c
ompares well with an independent measurement of gamma(LR).