Collapse of polymer brushes grafted onto planar ... - Wageningen UR
Collapse of polymer brushes grafted onto planar ... - Wageningen UR
Collapse of polymer brushes grafted onto planar ... - Wageningen UR
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COIL-SIZE OSCILLATORY PACKING IN POLYMER SOLUTIONS NEAR A S<strong>UR</strong>FACE<br />
J. van der Gucht, N.A.M. Besseling, J. van Male, M.A. Cohen Stuart<br />
Laboratory <strong>of</strong> Physical Chemistry and Colloid Science, <strong>Wageningen</strong> University,<br />
Dreijenplein 6, 6703 HB <strong>Wageningen</strong>, The Netherlands<br />
email: jasper@fenk.wau.nl<br />
ABSTRACT<br />
Depletion <strong>of</strong> <strong>polymer</strong>s at a surface has been studied extensively before. Theories predict that the segment<br />
concentration pr<strong>of</strong>ile decreases monotonously with decreasing distance to the surface 1,2) . Furthermore it is<br />
generally accepted that the only relevant lengthscale above the overlap concentration is the “blob size”. The<br />
coil size is believed to be irrelevant in this regime 1,2) . We have performed detailed calculations <strong>of</strong> the density<br />
pr<strong>of</strong>ile <strong>of</strong> nonadsorbing <strong>polymer</strong>s near a surface, using the theory developed by Scheutjens and Fleer 1) . Our<br />
results indicate that there is a damped oscillatory contribution to the density pr<strong>of</strong>ile. Both the period <strong>of</strong> the<br />
oscillations and the decay length are proportional to the size <strong>of</strong> the individual coils and are independent <strong>of</strong> the<br />
<strong>polymer</strong> concentration, also above the overlap concentration. This indicates that the size <strong>of</strong> the individual<br />
coils is still a relevant lengthscale above the overlap concentration. The oscillations are associated with a<br />
liquid-like layering <strong>of</strong> <strong>polymer</strong> coils near the surface. In dilute solutions no oscillations are observed, because<br />
the decay length <strong>of</strong> the oscillations is smaller than the depletion correlation length. This is similar to the<br />
behaviour <strong>of</strong> simple fluids, where the Fisher-Widom line marks the transition from monotonic to oscillatory<br />
decay <strong>of</strong> the density correlation function 3) . The Fisher-Widom line in <strong>polymer</strong> solutions is proportional to the<br />
overlap concentration. On the oscillatory side <strong>of</strong> the Fisher-Widom line the interaction energy between two<br />
plates immersed in a solution <strong>of</strong> nonadsorbing <strong>polymer</strong>s is an oscillatory function <strong>of</strong> the separation distance.<br />
The size <strong>of</strong> the oscillations is too small to be detected experimentally, but the effect is expected to be<br />
stronger in for example branched <strong>polymer</strong> solutions. As indicated by Evans et al. the oscillations might be <strong>of</strong><br />
importance in, for example, wetting phenomena 4) .<br />
References<br />
1. Fleer, G.J., Cohen Stuart, M.A., Scheutjens, J.M.H.M.; Cosgrove, T., Vincent, B. Polymers at Interfaces.<br />
Chapman and Hall: London, 1993.<br />
2. De Gennes, P.G., Scaling Concepts in Polymer Physics; Cornell University Press: Ithaca, London.<br />
3. Fisher, M.E., and Widom, B., 1969. J. Chem. Phys. 50, 3756.<br />
4. Evans, R., Leote de Carvalho, R.J.F., Henderson, J.R. and Hoyle, D.C., 1993. J. Chem. Phys., 100, 591.