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W. Richard Bowen and Nidal Hilal 4

W. Richard Bowen and Nidal Hilal 4

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1000 nm<br />

8.3 ENd-gRAFTEd POLyMER CHAINS 231<br />

500 nm<br />

0 nm 0 nm<br />

500 nm<br />

24.95 nm<br />

1000 nm<br />

FIgurE 8.4 AFM 3D-graph topography image of a gold substrate immersed in a toluene<br />

solution of PS-SH (concentration: 0.1 mg ml –1 , molecular weight: 144 000 g mol –1 ) for 45 min.<br />

The AFM imaging was conducted in water, which is a bad solvent for PS. The polymer chains<br />

are in collapsed globular state <strong>and</strong> r<strong>and</strong>omly distributed on the gold terraces.<br />

including simple geometrical formulas in order to estimate the true volume<br />

of the isl<strong>and</strong>s [18, 20]. The dimensions of polymer isl<strong>and</strong>s deduced<br />

directly from AFM images show an average height <strong>and</strong> width of about<br />

5.5 <strong>and</strong> 48 nm, respectively. As we have explained, although the measurement<br />

of height can be reliable, the width is usually overestimated<br />

owing to the convolution effect. Assuming that the shape of a polymer<br />

isl<strong>and</strong> is a spherical cap <strong>and</strong> taking into account the convolution effect,<br />

the average volume of the globules was estimated to be around 310 nm 3 .<br />

This compares well with the volume of a single collapsed polymer chain,<br />

which can be calculated assuming the usual bulk density for polystyrene<br />

(�1 g cm –3 ). Therefore, we conclude that the polymer isl<strong>and</strong>s are isolated<br />

single polymer chains chemisorbed <strong>and</strong> collapsed into dense globules<br />

onto the gold substrate. This implies that for this incubation time the<br />

polymer chains are sparsely distributed <strong>and</strong> the grafting density is low<br />

enough for us to observe the ‘mushroom’ regime. The variation in the<br />

size of the polymer globules reflects the polymer polydispersity (M w/<br />

M n� 1.2, where M n is the number-average molecular weight) <strong>and</strong> possibly<br />

small changes in the globular conformation, which can be magnified<br />

by the convolution effect.<br />

Figures 8.5 <strong>and</strong> 8.6 show two examples of gold substrates that<br />

were immersed in a toluene solution of higher concentration of PS-SH<br />

(2 mg ml –1 ) for much longer incubation times (2 days) <strong>and</strong> imaged under<br />

water in contact AFM mode. We can clearly see that the gold substrates<br />

are covered by a dense array of large polymer globules. Forty-eight hours<br />

is adequate time for the adsorption to reach its maximum grafting density,<br />

<strong>and</strong> we expect to have several thous<strong>and</strong>s of chains within a square

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