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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VOLUME FRACTION PROFILES OF ADSORBED POLYMER LAYERS<br />
T. Cosgrove 1) , J. Marshall 1) , J. Hone 1) , F. Leermakers 2) , T.M. Obey 1) , J. Marshall 1)<br />
1) University <strong>of</strong> Bristol, School <strong>of</strong> Chemistry,<br />
Cantock’s Close, Bristol BS8 1TS, United Kingdom<br />
2) Laboratory <strong>of</strong> Physical and Colloid Chemistry, <strong>Wageningen</strong> University,<br />
Dreijenplein 6, 6703 BC <strong>Wageningen</strong>, The Netherlands<br />
email: terence.cosgrove@bris.ac.uk<br />
ABSTRACT<br />
Volume fraction pr<strong>of</strong>iles for adsorbed <strong>polymer</strong>s are central to the understanding and manipulation <strong>of</strong> colloidal<br />
dispersions. Small-angle neutron scattering has proven to be an elegant method for determining the shape <strong>of</strong><br />
the volume fraction pr<strong>of</strong>ile though there are some difficulties in dealing with concentration fluctuations. In this<br />
presentation we shall develop the SANS methods for both on and <strong>of</strong>f contrast scattering and use it together<br />
with scaling and mean field theories to provide the most detailed shapes yet for adsorbed <strong>polymer</strong> layers on<br />
colloidal particles. The improvement in these methods due to better resolution in particle size and momentum<br />
transfer (Q) has made it possible to expand the studies to look at complex formation at interfaces with<br />
surfactants and sugars.<br />
Results and Discussion<br />
-1<br />
I(Q) /cm<br />
1<br />
0.1<br />
0.01<br />
Q /Å -1<br />
0.01 0.1<br />
Figure 1 Figure 2<br />
(z) φ<br />
0.1<br />
0.01<br />
0.001<br />
112.1 K PEO Exponential Pr<strong>of</strong>iles<br />
112.1 K PEO Scaling Pr<strong>of</strong>iles<br />
112.1 K PEO Scheutjens-Fleer Pr<strong>of</strong>iles<br />
0 50 100 150 200 250<br />
Figure 1 shows the scattering obtained from a deuterated polystyrene latex with adsorbed polyethylene oxide<br />
(110K Mw) suspended in water that has the same scattering length density as the latex. Under these<br />
circumstances the latex is essentially invisible. However, unlike earlier data we observe strong oscillation in<br />
the scattering from the <strong>polymer</strong> layer. This is partly due to preparing a very monodisperse latex (radii<br />
625 ± 20 Ã and 443 ± 10 Ã) and by obtaining higher Q resolution on the D22 camera at Grenoble and NG3 at<br />
NIST. The data have been fitted using an exponential volume fraction pr<strong>of</strong>ile with fluctuations (solid line) and<br />
without fluctuations (dashed line) both smeared for Q resolution. It is clear that fluctuations do contribute to<br />
the scattering and without suitable safeguards fitting the data without fluctuations can be problematical.<br />
z /Å<br />
R g 112.1 K PEO