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W. Richard Bowen and Nidal Hilal 4

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2.3 INTERACTION FORCES 55<br />

separations, deviations did occur. This was attributed by the authors to<br />

an effect of the roughness of the surfaces involved, leading to a deviation<br />

from the assumed idealised geometry.<br />

There are a number of examples of the AFM being used along with the<br />

colloidal probe technique to probe van der Waals interactions between<br />

surfaces in a variety of media. Whilst most such studies examine a combination<br />

of van der Waals along with other surface forces, there are a few<br />

that concentrate on van der Waals measurements. Milling <strong>and</strong> colleagues<br />

[76] observed the interactions between colloidal gold spheres <strong>and</strong> poly(tetrafluoroethylene)<br />

(PTFE) surfaces in a variety of different liquids. Hamaker<br />

constants were found by fitting the appropriate force laws to the experimental<br />

data. As noted by the authors, the experimentally determined<br />

values for the Hamaker constant were only in agreement qualitatively<br />

with those calculated from theory. In addition, theoretical values varied<br />

significantly, depending upon whether an amorphous or crystalline form<br />

of PTFE was considered. For the majority of liquids used, which were of<br />

a polar nature (water, ethanol <strong>and</strong> dimethyl sulfoxide), only attractive<br />

forces were measured. In the case of dimethyl formamide, which was also<br />

a polar molecule, only repulsive interactions were observed. For these<br />

interactions, only water had been expected to show an attractive interaction.<br />

The authors concluded that in the case of the other polar liquids<br />

studied that showed attraction, the surfaces must have become contaminated<br />

by charged groups, leading to interactions that were not purely of<br />

a van der Waals nature. For interactions taking place in the perfluoroalkanes<br />

perfluorohexane <strong>and</strong> perfluorocyclohexane, as well as in air, shortrange<br />

interactions were also attractive. This was as predicted from theory,<br />

but the authors were unable to obtain experimentally determined values<br />

for A H. In the other low-polarity solvents examined (cyclohexane, dodecane,<br />

p-xylene <strong>and</strong> bromobenzene), all interactions were found to be repulsive,<br />

which was qualitatively in accordance with theoretical A H values calculated<br />

assuming amorphous PTFE surfaces.<br />

Karamen et al. [77] studied the interactions between model aluminium<br />

oxide surfaces in 1 mM solutions of potassium chloride as a function of<br />

pH. At separation distances greater than 5 nm, interaction forces were<br />

described very well by the traditional DLVO theory. From calculations<br />

of the surface potential from forces measured using DLVO theory, it was<br />

possible to calculate an isoelectric point at approximately pH 7, which<br />

was in agreement with values obtained from the literature.<br />

Many colloidal systems consist of particles with self-assembled monolayers<br />

covalently bound to the surface. Such a system is inherently more<br />

complex than those having interactions between single materials, as if the<br />

outer layer is thin, then interactions between the underlying surfaces will<br />

occur as well as between the monolayers. Kane <strong>and</strong> Mulvaney [78] studied<br />

the interactions between gold spheres <strong>and</strong> surfaces before <strong>and</strong> after

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