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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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262 9. APPLICATION OF ATOMIC FORCE MICROSCOPy<br />

FIguRE 9.6 Formation of macroscopic viscoelastic liquid filaments formed in a filament<br />

stretching rheometer. The fluid is constrained between the ends of two cylinders, which are<br />

pulled apart at a specified rate. The generated tensile force <strong>and</strong> the filament profile are used<br />

to calculate the extensional stress. The cylinder shown is 10 mm in diameter.<br />

FIguRE 9.7 Images showing a typical CaBER experiment on a biopolymer solution.<br />

The surfaces are separated at a predetermined distance, thereafter the temporal evolution of<br />

the surface profile is used to determine rheological properties. Cylinder diameter is 2 mm.<br />

be extended. If the initial minimum separation distance is sub-micron<br />

<strong>and</strong> the retraction event is sufficiently rapid, then the stresses generated<br />

within the liquid may approach or exceed the tensile strength of the liquid.<br />

However, in AFM studies the fluid is not directly observed, therefore<br />

fluid draining, viscoelastic filamentatious behaviour or cavitational failure<br />

is not readily substantiated. It is, therefore, useful to examine those<br />

means by which the deforming liquid can be observed <strong>and</strong> documented.<br />

The separation distances considered in most AFM force studies are near<br />

to, or beyond, the limits of conventional optical microscopy. Although it<br />

is not possible to observe nanofilaments through an optical microscope,

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