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Instability and rupture of sheared viscous liquid nanofilms

Article dans une revue avec comité de lecture
Author
DHALIWAL, Vira
50791 University of Oslo [UiO]
PEDERSEN, Christian
50791 University of Oslo [UiO]
KADRI, Kheireddin
86289 Laboratoire Procédés et Ingénierie en Mécanique et Matériaux [PIMM]
ccMIQUELARD-GARNIER, Guillaume
86289 Laboratoire Procédés et Ingénierie en Mécanique et Matériaux [PIMM]
ccSOLLOGOUB, Cyrille
86289 Laboratoire Procédés et Ingénierie en Mécanique et Matériaux [PIMM]
ccPEIXINHO, Jorge
86289 Laboratoire Procédés et Ingénierie en Mécanique et Matériaux [PIMM]
ccSALEZ, Thomas
136813 Laboratoire Ondes et Matière d'Aquitaine [LOMA]
CARLSON, Andreas
50791 University of Oslo [UiO]

URI
http://hdl.handle.net/10985/25544
DOI
10.1103/physrevfluids.9.024201
Date
2024-02
Journal
Physical Review Fluids

Abstract

Liquid nanofilms are ubiquitous in nature and technology, and their equilibrium and out-of-equilibrium dynamics are key to a multitude of phenomena and processes. We numerically study the evolution and rupture of viscous nanometric films, incorporating the effects of surface tension, van der Waals forces, thermal fluctuations, and viscous shear. We show that thermal fluctuations create perturbations that can trigger film rupture, but they do not significantly affect the growth rate of the perturbations. The film rupture time can be predicted from a linear stability analysis of the governing thin film equation, by considering the most unstable wavelength and the thermal roughness. Furthermore, applying a sufficiently large unidirectional shear can stabilize large perturbations, creating a finite-amplitude traveling wave instead of film rupture. In three dimensions, unidirectional shear does not inhibit rupture, as perturbations are not suppressed in the direction perpendicular to the applied shear. However, if the direction of shear varies in time, then the growth of large perturbations is prevented in all directions, and rupture can be impeded. © 2024 American Physical Society.

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