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Thermocapillary long waves in a liquid film flow. Part 2. Linear stability and nonlinear waves

Published online by Cambridge University Press:  17 August 2005

B. SCHEID
Affiliation:
Chimie-Physique E.P., Université Libre de Bruxelles, C.P. 165/62, 1050 Brussels, Belgiumbscheid@ulb.ac.be Laboratoire FAST, UMR 7608, CNRS, Universités P. et M. Curie et Paris Sud, Bât. 502, Campus Universitaire, 91405 Orsay Cedex, Franceruyer@fast.u-psud.fr
C. RUYER-QUIL
Affiliation:
Laboratoire FAST, UMR 7608, CNRS, Universités P. et M. Curie et Paris Sud, Bât. 502, Campus Universitaire, 91405 Orsay Cedex, Franceruyer@fast.u-psud.fr
S. KALLIADASIS
Affiliation:
Department of Chemical Engineering, University of Leeds, Leeds LS2 9JT, UKs.kalliadasis@imperial.ac.uk Present address: Department of Chemical Engineering, Imperial College, London SW7 2AZ, UK.
M. G. VELARDE
Affiliation:
Insituto Pluridisciplinar, Universidad Complutense de Madrid, Paseo Juan XXIII, n. 1, E-28040 Madrid, Spainvelarde@fluidos.pluri.ucm.es
R. Kh. ZEYTOUNIAN
Affiliation:
Université des Sciences et Technologies de Lille, 59655 Villeneuve d'Asq cédex, Francezeytounian@aol.com

Abstract

We analyse the regularized reduced model derived in Part 1 (Ruyer-Quil et al. 2005). Our investigation is two-fold: (i) we demonstrate that the linear stability properties of the model are in good agreement with the Orr–Sommerfeld analysis of the linearized Navier–Stokes/energy equations; (ii) we show the existence of nonlinear solutions, namely single-hump solitary pulses, for the widest possible range of parameters. We also scrutinize the influence of Reynolds, Prandtl and Marangoni numbers on the shape, speed, flow patterns and temperature distributions for the solitary waves obtained from the regularized model. The hydrodynamic and Marangoni instabilities are seen to reinforce each other in a non-trivial manner. The transport of heat by the flow has a stabilizing effect for small-amplitude waves but promotes the instability for large-amplitude waves when a recirculating zone is present. Nevertheless, in this last case, by increasing the shear in the bulk and thus the viscous dissipation, increasing the Prandtl number decreases the amplitude and speed of the waves.

Type
Papers
Copyright
© 2005 Cambridge University Press

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