W. Richard Bowen and Nidal Hilal 4
W. Richard Bowen and Nidal Hilal 4
W. Richard Bowen and Nidal Hilal 4
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178 6. NANOSCALE ANALySIS Of PHARMACEUTICALS by SCANNINg PRObE MICROSCOPy<br />
These <strong>and</strong> other studies can broadly be divided into two types: those<br />
that rank relative particulate interactions <strong>and</strong> those that attempt to make<br />
a quantitative comparison of force per unit area of contact. Ranking studies<br />
address, e.g., how drug-drug cohesion compares to drug-excipient<br />
particle <strong>and</strong> drug-device adhesion. Since particulate interactions are dominated<br />
by aspects such as surface morphology, surface roughness, exposed<br />
chemical moieties <strong>and</strong> thermodynamic properties, all of which can vary<br />
from particle to particle <strong>and</strong> indeed within a single particle, such ranking<br />
comparisons are normally made using the same particle to challenge<br />
all the possible combinations of interactions. In this case, ranking should<br />
be consistent for each drug particle probe, but the absolute values of adhesion<br />
force determined cannot be used to make comparisons from particle<br />
to particle or between materials [18].<br />
To quantify such measurements, particle variability <strong>and</strong> a lack of direct<br />
knowledge of the contacting regions must be overcome to allow the<br />
determination of factors such as surface energy <strong>and</strong> work of adhesion.<br />
The use of AFM to determine such properties on model flat surfaces, such<br />
as silicon, was established relatively early [25]. However, its application<br />
to pharmaceuticals due to difficulties of rough <strong>and</strong> variable particle morphology<br />
came later [19, 21, 22]. In these works, the principal variable that<br />
is allowed for is contact area. Contact areas have, to date, been estimated<br />
either via a direct imaging approach [22] or indirectly through imaging<br />
indents made by the particle probe in a plastic polymer film [19]. The<br />
subsequent use of adhesion models such as Johnson–Kendall–Roberts<br />
<strong>and</strong> Derjaguin–Muller–Toporov can then allow the surface energy of the<br />
particle (over the region of contact) to be determined. In this way, e.g.,<br />
micronised (milled) salbutamol sulphate <strong>and</strong> a version prepared via a<br />
novel supercritical fluid method have been compared [22].<br />
An alternative to this approach of trying to model the variable contact<br />
region between particles is to compare ratios of cohesive <strong>and</strong> adhesive<br />
forces between different particles rather than actual separation forces.<br />
This has allowed an assessment for relatively flat crystals of the affinity<br />
of salbutamol sulphate to lactose <strong>and</strong> budesonide to lactose, showing<br />
that salbutamol sulphate has a stronger affinity for lactose [26]. This<br />
information was then related successfully to the likely blend uniformity<br />
these materials would form.<br />
In addition to monitoring force normal to a surface, AFM is also capable<br />
of assessing frictional forces between a probe <strong>and</strong> a surface. This is<br />
achieved by recording the twist of the cantilever in addition to its vertical<br />
bend as it scans a surface in continuous contact with that surface<br />
(Figure 6.3a). This approach has recently been used to obtain singleparticle<br />
friction measurements on DPI formulations [27] <strong>and</strong> blister<br />
packaging material (used in DPIs) [28] <strong>and</strong> provides an opportunity to<br />
consider sliding as well as separation forces. Figure 6.3 shows examples