Ar. Esker et al., Dilational viscoelastic behaviors of homopolymer monolayers: surface lightscattering analysis, COLL SURF A, 171(1-3), 2000, pp. 131-148
Citations number
52
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
COLLOIDS AND SURFACES A-PHYSICOCHEMICAL AND ENGINEERING ASPECTS
This is to report a new set of viscoelastic analyses of common polymers tha
t are surface active at the air/water interface (A/W). The materials are po
lyethers such as poly(ethyleneoxide) (PEO) and poly(tetrahydrofuran) (PTHF)
, and vinyl polymers with pendant ester groups such as poly(vinylacetate) (
PVAc), poly(methylacrylate) (PMA), poly(methylmethacrylate) (PMMA) and poly
(t-butylmethacrylate) (PtBMA). Experimentally the viscoelastic parameters a
re deduced from the propagation characteristics of spontaneously formed cap
illary waves obtained by surface light scattering in conjunction with surfa
ce pressure II measurements by the Wilhelmy plate technique. The static fea
tures of polymer monolayers at A/W are delineated by the surface pressure d
ependence of the static dilational elasticity epsilon(s). Two static limits
are expected for the dependence, one being the good solvent condition and
the other the theta condition. By sorting polymers according to their stati
c features, these polymers fall into two groups, i.e. the good and poor sol
vent (not quite theta) groups. In this report, there is a clear corresponde
nce between the static features and viscoelastic characteristics of these p
olymer monolayers, and each group has its own differentiative static and vi
scoelastic profiles. The polymer monolayers belonging to the good solvent c
ondition exhibit a viscoelastic profile characterizable as nearly perfectly
elastic behavior over a wide range of surface coverage from infinite dilut
ion to II approximate to 4 mN m(-1). In contrast, those polymer monolayers
under poor solvent conditions, i.e. PMMA and PtBMA, show a viscoelastic pro
file of incompressible films with the dynamics approaching the limit of an
infinite lateral modulus, epsilon* --> infinity. (C) 2000 Elsevier Science
B.V. All rights reserved.