Hostname: page-component-8448b6f56d-tj2md Total loading time: 0 Render date: 2024-04-19T20:44:32.755Z Has data issue: false hasContentIssue false

Interfacial pattern selection in defiance of linear growth

Published online by Cambridge University Press:  19 September 2017

Jason R. Picardo
Affiliation:
Department of Chemical Engineering, Indian Institute of Technology Madras, Chennai, TN 600036, India Department of Chemical Engineering, University of Florida, Gainesville, Fl 32608, USA
R. Narayanan
Affiliation:
Department of Chemical Engineering, University of Florida, Gainesville, Fl 32608, USA

Abstract

In this study, we revisit Rayleigh’s visionary hypothesis (Rayleigh, Proc. R. Soc. Lond., vol. 29, 1879a, pp. 71–97), that patterns resulting from interfacial instabilities are dominated by the fastest-growing linear mode, as we study nonlinear pattern selection in the context of a linear growth (dispersion) curve that has two peaks of equal height. Such a system is obtained in a physical situation consisting of two liquid layers suspended from a heated ceiling, and exposed to a passive gas. Both interfaces are then susceptible to thermocapillary and Rayleigh–Taylor instabilities, which lead to rupture/pinch off via a subcritical bifurcation. The corresponding mathematical model consists of long-wavelength evolution equations which are amenable to extensive numerical exploration. We find that, despite having equal linear growth rates, either one of the peak-modes can completely dominate the other as a result of nonlinear interactions. Importantly, the dominant peak continues to dictate the pattern even when its growth rate is made slightly smaller, thereby providing a definite counter-example to Rayleigh’s conjecture. Although quite complex, the qualitative features of the peak-mode interaction are successfully captured by a low-order three-mode ordinary differential equation model based on truncated Galerkin projection. Far from being governed by simple linear theory, the final pattern is sensitive even to the phase difference between peak-mode perturbations. For sufficiently long domains, this phase effect is shown to result in the emergence of coexisting patterns, wherein each peak-mode dominates in a different region of the domain.

Type
Papers
Copyright
© 2017 Cambridge University Press 

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Balmforth, N. J., Provenzale, A. & Whitehead, J. A. 2001 The language of pattern and form. In Geomorphological Fluid Mechanics (ed. Balmforth, N. J. & Provenzale, A.), Springer.CrossRefGoogle Scholar
Busse, F. H. 1978 Non-linear properties of thermal convection. Rep. Prog. Phys. 41, 19291967.CrossRefGoogle Scholar
Carini, M., Auteri, F. & Giannetti, F. 2015 Centre-manifold reduction of bifurcating flows. J. Fluid Mech. 767, 109145.CrossRefGoogle Scholar
Cross, M. C. & Hohenberg, P. C. 1993 Pattern formation outside of equilibrium. Rev. Mod. Phys. 65 (3), 8511112.Google Scholar
Dauby, P. C., Colinet, P. & Johnson, D. 2000 Theoretical analysis of a dynamic thermoconvective pattern in a circular container. Phys. Rev. E 61, 26632668.Google Scholar
Dietze, G. F. & Ruyer-Quil, C. 2013 Wavy liquid films in interaction with a confined laminar gas flow. J. Fluid Mech. 722, 348393.Google Scholar
Echebarria, B., Krmpotic, D. & Perez-Garcia, C. 1997 Resonant interactions in Bénard–Marangoni convection in cylindrical containers. Physica D 99, 487502.Google Scholar
Eggers, J. 1997 Nonlinear dynamics and breakup of free-surface flows. Rev. Mod. Phys. 69, 865930.Google Scholar
Israelachvili, J. N. 2011 Intermolecular and Surface Forces, 3rd edn. Academic.Google Scholar
Johns, L. E. & Narayanan, R. 2002 Interfacial Instability. Springer.Google Scholar
Johnson, D. & Narayanan, R. 1996 Experimental observation of dynamic mode switching in interfacial-tension-driven convection near a codimension-two point. Phys. Rev. E 54 (4), R3102R3104.Google Scholar
Nepomnyashchy, A. A. & Simanovskii, I. B. 2007 Marangoni instability in ultrathin two-layer films. Phys. Fluids 19 (12), 122103.Google Scholar
Nepomnyashchy, A. A. & Simanovskii, I. B. 2012 Nonlinear marangoni waves in a two-layer film in the presence of gravity. Phys. Fluids 24 (3), 032101.Google Scholar
Nepomnyashchy, A., Simanovskii, I. & Legros, J. C. 2012 Interfacial Convection in Multilayer Systems, 2nd edn. Springer.Google Scholar
Oron, A, Davis, S. H. & Bankoff, S. G. 1997 Long-scale evolution of thin liquid films. Rev. Mod. Phys. 69 (3), 931980.Google Scholar
Pozrikidis, C. 1999 Capillary instability and breakup of a viscous thread. J. Engng Maths 36, 255275.Google Scholar
Proctor, M. R. E. & Jones, C. A. 1988 The interaction of two spatially resonant patterns in thermal convection. Part 1. Exact 1:2 resonance. J. Fluid Mech. 188, 301335.Google Scholar
Raitt, D. & Riecke, H. 1995 Domain structures in fourth-order phase and Ginzburg–Landau equations. Physica D 82 (1), 7994.Google Scholar
Raitt, D. & Riecke, H. 1997 Parametric forcing of waves with a nonmonotonic dispersion relation: domain structures in ferrofluids. Phys. Rev. E 55, 54485454.Google Scholar
Rayleigh, Lord 1879a On the capillary phenomena of jets. Proc R. Soc. Lond. 29, 7197.Google Scholar
Rayleigh, Lord 1879b On the instability of liquid jets. Proc. Lond. Math. Soc. 10, 413.Google Scholar
Roberts, A. J. 2015 Model Emergent Dynamics in Complex Systems. SIAM.Google Scholar
Ruyer-Quil, C. & Manneville, P. 2000 Improved modeling of flows down inclined planes. Eur. Phys. J. B 15 (2), 357369.Google Scholar
Yiantsios, S. G. & Higgins, B. G. 1989 Rayleigh–Taylor instability in thin viscous films. Phys. Fluids 1 (9), 14841501.Google Scholar