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W. Richard Bowen and Nidal Hilal 4

W. Richard Bowen and Nidal Hilal 4

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184 6. NANOSCALE ANALySIS Of PHARMACEUTICALS by SCANNINg PRObE MICROSCOPy<br />

FIgure 6.5 A sequence of 10 �m � 10 �m AFM images of the (001) face of a paracetamol<br />

crystal during incubation in paracetamol solution. In image (a) time t � 0 s, (b) t � 60 s,<br />

(c) t � 118 s, (d) t � 176 s, (e) t � 234 s <strong>and</strong> (f) t � 292 s. Figure reproduced with permission [46].<br />

shown in Figure 6.5, <strong>and</strong> illustrates that the growth steps of crystallisation<br />

over 4.8 h are curved in appearance, indicative of crystal growth via<br />

the screw dislocation mechanism. AFM images of the (001) face of another<br />

paracetamol crystal during incubation with 4 mol% acetanilide over time<br />

are shown in Figure 6.6. The defects in the crystal surface form weak<br />

points, leading to deepened holes (one hole is highlighted by a black<br />

arrow in Figure 6.6) over 12 h, indicating that the dissolution occurs both<br />

laterally <strong>and</strong> towards the crystal core [46]. Images during incubation with<br />

4 mol% metacetamol showed that the steps formed were significantly<br />

smaller <strong>and</strong> pointed in appearance (image not shown here). These features<br />

were ascribed to ‘pinning’, an effect caused when additives adsorb<br />

onto the steps <strong>and</strong> force them to grow between the impurities [46].<br />

From our consideration of AFM as a force measurement tool, it is clear<br />

that the probe is sensitive not only to topography but also to the magnitude<br />

<strong>and</strong> nature of the forces experienced by the probe. Consequently,<br />

whilst imaging, if such sensitivity can be mapped also, it becomes possible<br />

to produce alongside topography data sensitive to a particular surface<br />

property (e.g. adhesion, harness etc.). For example, during the commonly<br />

employed tapping mode imaging [47], where the AFM cantilever is oscillated<br />

at its resonant frequency <strong>and</strong> intermittently contacts a sample surface<br />

at the bottom of each oscillation cycle, the phase of the oscillation as well as

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