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W. Richard Bowen and Nidal Hilal 4

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120 4. INvEsTIgATINg MEMbRANEs ANd MEMbRANE PROCEssEs<br />

Moreover, if the surface potential or surface charge of the colloid has<br />

been determined <strong>and</strong> the solution is of defined ionic content, it is possible<br />

to calculate the potential or charge of the surface under investigation<br />

by matching the experimentally obtained curves to theoretical calculations<br />

on the basis of electrical double layer theory. In the example shown,<br />

the best-fit membrane surface charge was �0.00114 C m �2 <strong>and</strong> the bestfit<br />

membrane surface potential was �64 mV. Furthermore, an important<br />

advantage of the colloid probe technique is that it allows exploration<br />

of variations in surface electrical interactions at different points on the<br />

membrane surface, as the following section shows.<br />

4.5 EFFECTS OF SURFACE ROUghnESS On<br />

InTERACTIOnS WITh PARTICLES<br />

Surfaces are usually imaged using sharp tips in order to produce<br />

images with the highest possible definition. However, from a processing<br />

viewpoint, an important factor is how process stream components such as<br />

solutes <strong>and</strong> colloidal particles interact with the surface. If a surface has feature<br />

variations that have dimensions comparable with those of the process<br />

stream components, then such interactions may show variations at different<br />

locations on the surface. An effective way of gauging such effects is to<br />

image the surface with an appropriate stream component, e.g. a particle<br />

that is immobilised to form a colloid probe. Figure 4.14 shows results for<br />

a reverse osmosis membrane (AFC99, PCI Membranes) imaged in saline<br />

solution with first a sharp tip <strong>and</strong> then a 4.2 �m silica sphere [8].<br />

µm<br />

0.4<br />

0.2<br />

4<br />

0<br />

3<br />

P–v = 560 nm<br />

Rms = 66nm<br />

2<br />

µm<br />

1 1<br />

0 0<br />

2<br />

µm<br />

A B<br />

3<br />

4<br />

µm<br />

0.16<br />

0.12<br />

0.2<br />

0.04<br />

4<br />

0<br />

3<br />

2<br />

µm<br />

P–v = 186 nm<br />

Rms = 21nm<br />

1 1<br />

0 0<br />

FIgURE 4.14 AFC99 membrane imaged with a tip (A) <strong>and</strong> with a 4.2 �m colloid probe<br />

(B) (P–v, peak to valley; Rms, root mean square).<br />

2<br />

µm<br />

3<br />

4

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