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W. Richard Bowen and Nidal Hilal 4

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

where k is the cantilever force constant, � the ratio of cantilever to substrate<br />

modulation amplitude <strong>and</strong> φ the phase angle between substrate<br />

<strong>and</strong> cantilever response. It is important to note that the equivalence of<br />

the phase terms φ <strong>and</strong> � is not always physically representative, <strong>and</strong> a<br />

quantitative description of the rheological properties of a homogeneous<br />

fluid sample may be verified under some conditions; however, when the<br />

sample fluid is non-uniform, e.g. an adsorbed polymer layer is present,<br />

only qualitative information can be obtained.<br />

9.4 DETERMInATIon oF RhEoLogICAL PRoPERTIES<br />

FRoM RESonAnCE SPECTRA<br />

The resonance characteristics of microcantilevers immersed in fluids<br />

have long been recognised as a potential basis for rheometrical microsensor<br />

technology as the resonance spectra of a vibrating cantilever are<br />

influenced by the viscosity <strong>and</strong> density of the surrounding medium.<br />

Compared to vibration in air, the fundamental resonant frequency of a<br />

rectangular cantilever is reduced when operated in liquid; immersion<br />

in increasingly more viscous liquids reduces the resonant frequency<br />

further – this is accompanied by a broadening of the resonant peak <strong>and</strong> a<br />

decrease in peak amplitude (Figure 9.5).<br />

The shift in the mechanical response is attributed to the viscous<br />

drag <strong>and</strong> inertial effects caused by the fluid adjacent to the cantilever. The<br />

resonance characteristics are often derived from the effect of environmental<br />

stimuli – most commonly thermally induced vibrations. The thermal<br />

noise spectrum is derived from the Fourier transform of the displacement<br />

of the cantilever. Fast Fourier transforms (FFTs) are routinely used<br />

in sound <strong>and</strong> vibration analysis to convert a signal from a time domain to<br />

A<br />

High viscosity<br />

ω<br />

Low viscosity<br />

FIguRE 9.5 Resonance frequency shift due to immersion in viscous fluids.

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