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W. Richard Bowen and Nidal Hilal 4

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

measurements more typically measured on a micron or greater scale to<br />

determine elastic modulus <strong>and</strong> hardness [29]. There are, however, a number<br />

of limitations of the AFM data that must first be considered. First,<br />

as st<strong>and</strong>ard AFM cantilevers are typically very flexible (so that they are<br />

sensitive to nanoNewton forces), they are incapable of deforming surfaces<br />

beyond approximately 10 GPa elastic modulus. Second, unlike a<br />

traditional indenter, an AFM probe does not approach or deform a surface<br />

completely normal to that surface, because of the need to have the<br />

lever at a slight angle to ensure that the probe apex contacts the sample<br />

first. This causes lateral deformation errors in the data, which are only<br />

negligible with relatively small indent depths.<br />

Despite these issues, many groups have employed AFM to determine the<br />

elastic, inelastic <strong>and</strong> hardness properties of materials. Such deformation<br />

behaviour of pharmaceutical ingredients is known to affect pharmaceutical<br />

processes such as milling <strong>and</strong> compaction [30–33]. To date, most<br />

reported pharmaceutical examples of this approach have used a modified<br />

AFM equipped with a relatively large probe with well-defined<br />

geometry <strong>and</strong> a much stiffened spring that supports this probe [30,<br />

34, 35]. Typically, in these methods, material parameters are extracted<br />

from load-displacement unloading curves using approaches outlined by<br />

Oliver <strong>and</strong> Pharr [36]. Recently, Ward <strong>and</strong> co-workers [37] have utilised<br />

a sharp AFM probe <strong>and</strong> normal cantilevers to record nanomechanical<br />

measurements on sorbital samples to quantitatively distinguish between<br />

amorphous <strong>and</strong> crystalline domains through Young’s modulus measurements.<br />

Figure 6.4 shows images <strong>and</strong> typical force distance curves<br />

obtained from crystalline <strong>and</strong> amorphous sorbitol regions <strong>and</strong> a control<br />

of a hard, non-indenting silicon substrate. To determine the nanoindentation<br />

of the probe tip into the sorbitol sample as a function of load,<br />

the force distance curves from the sorbitol sample <strong>and</strong> the control hard<br />

substrate were compared. When comparing the amorphous <strong>and</strong> the<br />

crystalline regions, it is the amorphous region that provided the greater<br />

deflection of the tip (indicating the softer material <strong>and</strong> greater indentation)<br />

at the given applied loads [37]. In this approach, a comparison of<br />

the gradients of the contact region of the force distance curves between<br />

a hard non-deformable reference surface <strong>and</strong> the sample can provide the<br />

relative stiffness of a surface [38]. By applying the Hertz model [39] to<br />

the nanoindentation data, a quantitative value of the Young’s modulus of<br />

the surfaces can be obtained. The Hertz model describes the elastic deformation<br />

of two homogenous surfaces under an applied load <strong>and</strong> is often<br />

used to model AFM data since it requires little knowledge of parameters<br />

such as surface energy. The first step in modelling the data is to compare<br />

force distance curves recorded on the sample <strong>and</strong> an ideally hard reference<br />

(glass surface) to determine the indentation (�) of the probe into the<br />

sample as a function of load. The contact regions of the curves are overlaid<br />

such that zero force is equal to zero indentation.

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