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W. Richard Bowen and Nidal Hilal 4

W. Richard Bowen and Nidal Hilal 4

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LIST OF SyMbOLS 269<br />

instance it is intended to conduct additional microscopic observations from<br />

beneath the liquid layer. In this way, the current restrictions imposed by the<br />

focal distance can be reduced (it is necessary to use ULWD dry lenses to<br />

document filament formation), <strong>and</strong> high numerical aperture oil immersion<br />

lenses may be employed to study microscale cavitational effects in the thin<br />

fluid layer prior to the mesoscale deformation process.<br />

ACknowLEDgEMEnTS<br />

The authors would like to acknowledge Prof. W. <strong>Richard</strong> <strong>Bowen</strong> <strong>and</strong><br />

Prof. <strong>Nidal</strong> <strong>Hilal</strong> for their significant contribution to the research content<br />

presented in section 9.6. The authors are grateful for the financial support<br />

of the EPSRC, the work reported here was conducted under EPSRC grant<br />

no. GR/S10438/01.<br />

LIST oF SyMBoLS<br />

A Cantilever vibration amplitude m<br />

an Constant<br />

B Geometric apparatus coefficient m<br />

bp Viscous damping coefficient N s m�1 F Force N<br />

G* Complex modulus Pa<br />

G’′ Elastic modulus Pa<br />

G“″ Viscous modulus Pa<br />

H Separation distance between probe <strong>and</strong> surface m<br />

K Spring constant N m�1 R Radius of sphere m<br />

T Cantilever thickness m<br />

U Relative separation velocity m s�1 X Cantilever width m<br />

Z Displacement m<br />

� Ratio of cantilever <strong>and</strong> drive amplitude<br />

�circ Hydrodynamic function for cylindrical cantilever<br />

�rect Hydrodynamic function for rectangular<br />

cantilever<br />

� Rheological phase angle °

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