Transient two-dimensional coating flow of a viscoelastic fluid film on a substrate of arbitrary shape

Authors
Citation
Re. Khayat, Transient two-dimensional coating flow of a viscoelastic fluid film on a substrate of arbitrary shape, J NON-NEWT, 95(2-3), 2000, pp. 199-233
Citations number
35
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Mechanical Engineering
Journal title
JOURNAL OF NON-NEWTONIAN FLUID MECHANICS
ISSN journal
03770257 → ACNP
Volume
95
Issue
2-3
Year of publication
2000
Pages
199 - 233
Database
ISI
SICI code
0377-0257(200012)95:2-3<199:TTCFOA>2.0.ZU;2-U
Abstract
The interplay between inertia and viscoelasticity, as well as the influence of gravity and substrate topography are examined in this study for the tra nsient two-dimensional flow of a thin film. The fluid is assumed to emerge from a channel, as it is driven by a pressure gradient, which is maintained inside the channel. The substrate is assumed to be stationary. The lubrica tion equations are generalized for a viscoelastic fluid obeying the Oldroyd -B constitutive model. These equations are solved by expanding the flow fie ld in Fourier modes in the vertical direction and using the Galerkin projec tion, combined with a time-stepping implicit scheme, and integration along the flow direction. It is found that the viscosity ratio, fluid elasticity, gravity and substrate topography can have a significant effect on transien t behavior, but this effect varies significantly, depending on the level of fluid inertia. The wave and flow structures are examined for high- and low -inertia fluids. It is found that low-inertia and/or highly elastic fluids tend to accumulate near the channel exit, exhibiting a standing wave that g rows with time. This behavior clearly illustrates the difficulty faced with coating viscoelastic high-viscosity fluids. In the presence of gravity, st eady-state conditions are observed to be difficult to reach, even near the channel exit. The topography of the substrate has a drastic effect on the f low. A secondary wave emerges in the presence of a bump or a depression in the substrate. The wave structure is again highly dependent on the level of inertia. (C) 2000 Elsevier Science B.V. All rights reserved.