It is known that the spreading rates of small liquid
drops over a solid surface exhibit a
strong dependence on the viscosity of the liquid. These
observations have led us to study the spreading
behavior of polymer solutions on high- and low-energy substrates to
determine what role complex rheology
plays in wetting kinetics. We did not observe any effects of
non-Newtonian (nonlinear) behavior, nor
were any obvious signs of viscoelasticity (memory) visible.
Instead, we observed a most intriguing
phenomenon that polymer solutions, despite having low surface energies,
do not wet high-energy
substrates. In addition, nonwetting drops spread to an equilibrium
configuration by either one of two
distinct mechanisms. In the first case, they spread as a wetting
Newtonian liquid and then stopped,
that is, equilibrated, abruptly. In the second, they equilibrated
continuously. We offer some possible
molecular and continuum arguments to explain the differences between
these two mechanisms.
The onset of significant departure from isothermality caused by viscous energy dissipation in flow through a slit is determined for isothermal and adiabatic walls. A series solution of the energy equation enables calculation of dimensionless profiles for any power law fluid. Such solutions provide useful standards for judging performances of numerical schemes for solving complex nonisothermal flows.
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