Imperial College London
Alternate

ProfessorDemetriosPapageorgiou

Faculty of Natural Sciences, Department of Mathematics

Chair in Applied Maths and Mathematical Physics
 
 
 
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Contact

 

+44 (0)20 7594 8369d.papageorgiou Website

 
 
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Location

 

750Huxley BuildingSouth Kensington Campus

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Summary

 

Publications

Citation

BibTex format

@article{Kalogirou:2016:10.1017/jfm.2016.429,
author = {Kalogirou, A and Papageorgiou, DT},
doi = {10.1017/jfm.2016.429},
journal = {Journal of Fluid Mechanics},
pages = {5--36},
title = {Nonlinear dynamics of surfactant-laden two-fluid Couette flows in the presence of inertia},
url = {http://dx.doi.org/10.1017/jfm.2016.429},
volume = {802},
year = {2016}
}
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RIS format (EndNote, RefMan)

TY  - JOUR
AB  - The nonlinear stability of immiscible two-fluid Couette flows in the presence of inertia is considered. The interface between the two viscous fluids can support insoluble surfactants and the interplay between the underlying hydrodynamic instabilities and Marangoni effects is explored analytically and computationally in both two and three dimensions. Asymptotic analysis when one of the layers is thin relative to the other yields a coupled system of nonlinear equations describing the spatio-temporal evolution of the interface and its local surfactant concentration. The system is non-local and arises by appropriately matching solutions of the linearised Navier–Stokes equations in the thicker layer to the solution in the thin layer. The scaled models are used to study different physical mechanisms by varying the Reynolds number, the viscosity ratio between the two layers, the total amount of surfactant present initially and a scaled Péclet number measuring diffusion of surfactant along the interface. The linear stability of the underlying flow to two- and three-dimensional disturbances is investigated and a Squire’s type theorem is found to hold when inertia is absent. When inertia is present, three-dimensional disturbances can be more unstable than two-dimensional ones and so Squire’s theorem does not hold. The linear instabilities are followed into the nonlinear regime by solving the evolution equations numerically; this is achieved by implementing highly accurate linearly implicit schemes in time with spectral discretisations in space. Numerical experiments for finite Reynolds numbers indicate that for two-dimensional flows the solutions are mostly nonlinear travelling waves of permanent form, even though these can lose stability via Hopf bifurcations to time-periodic travelling waves. As the length of the system (that is the wavelength of periodic waves) increases, the dynamics becomes more complex and includes time-periodic, quasi-periodic
AU  - Kalogirou,A
AU  - Papageorgiou,DT
DO  - 10.1017/jfm.2016.429
EP  - 36
PY  - 2016///
SN  - 1469-7645
SP  - 5
TI  - Nonlinear dynamics of surfactant-laden two-fluid Couette flows in the presence of inertia
T2  - Journal of Fluid Mechanics
UR  - http://dx.doi.org/10.1017/jfm.2016.429
UR  - http://hdl.handle.net/10044/1/40335
VL  - 802
ER  -
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