Two-layer electrified pressure-driven flow in topographically structured channels
File(s)PAPER-revised-11-2016.pdf (1.18 MB)
Accepted version
Author(s)
Dubrovina, E
Craster, RV
Papageorgiou, DT
Type
Journal Article
Abstract
The flow of two stratified viscous immiscible perfect dielectric fluids in a channel with
topographically structured walls is investigated. The flow is driven by a streamwise
pressure gradient and an electric field across the channel gap. This problem is
explored in detail by deriving and studying a nonlinear evolution equation for the
interface valid for large-amplitude long waves in the Stokes flow regime. For flat
walls, the electrified flow is long-wave unstable with a critical cutoff wavenumber
that increases linearly with the magnitude of the applied voltage. In the nonlinear
regime, it is found that the presence of pressure-driven flow prevents electrostatically
induced interface touchdown that has been observed previously – time-modulated
nonlinear travelling waves emerge instead. When topography is present, linearly stable
uniform flows become non-uniform spatially periodic steady states; a small-amplitude
asymptotic theory is carried out and compared with computations. In the linearly
unstable regime, intricate nonlinear structures emerge that depend, among other
things, on the magnitude of the wall corrugations. For a low-amplitude sinusoidal
boundary, time-modulated travelling waves are observed that are similar to those
found for flat walls but are influenced by the geometry of the wall and slide over it
without touching. The flow over a high-amplitude sinusoidal pattern is also examined
in detail and it is found that for sufficiently large voltages the interface evolves to
large-amplitude waves that span the channel and are subharmonic relative to the wall.
A type of ‘walking’ motion emerges that causes the lower fluid to wash through the
troughs and create strong vortices over the peaks of the lower boundary. Non-uniform
steady states induced by the topography are calculated numerically for moderate and
large values of the flow rate, and their stability is analysed using Floquet theory.
The effect of large flow rates is also considered asymptotically to find solutions that
compare very well with numerical computations.
topographically structured walls is investigated. The flow is driven by a streamwise
pressure gradient and an electric field across the channel gap. This problem is
explored in detail by deriving and studying a nonlinear evolution equation for the
interface valid for large-amplitude long waves in the Stokes flow regime. For flat
walls, the electrified flow is long-wave unstable with a critical cutoff wavenumber
that increases linearly with the magnitude of the applied voltage. In the nonlinear
regime, it is found that the presence of pressure-driven flow prevents electrostatically
induced interface touchdown that has been observed previously – time-modulated
nonlinear travelling waves emerge instead. When topography is present, linearly stable
uniform flows become non-uniform spatially periodic steady states; a small-amplitude
asymptotic theory is carried out and compared with computations. In the linearly
unstable regime, intricate nonlinear structures emerge that depend, among other
things, on the magnitude of the wall corrugations. For a low-amplitude sinusoidal
boundary, time-modulated travelling waves are observed that are similar to those
found for flat walls but are influenced by the geometry of the wall and slide over it
without touching. The flow over a high-amplitude sinusoidal pattern is also examined
in detail and it is found that for sufficiently large voltages the interface evolves to
large-amplitude waves that span the channel and are subharmonic relative to the wall.
A type of ‘walking’ motion emerges that causes the lower fluid to wash through the
troughs and create strong vortices over the peaks of the lower boundary. Non-uniform
steady states induced by the topography are calculated numerically for moderate and
large values of the flow rate, and their stability is analysed using Floquet theory.
The effect of large flow rates is also considered asymptotically to find solutions that
compare very well with numerical computations.
Date Issued
2017-02-02
Date Acceptance
2016-12-30
Citation
Journal of Fluid Mechanics, 2017, 814, pp.222-248
ISSN
0022-1120
Publisher
Cambridge University Press
Start Page
222
End Page
248
Journal / Book Title
Journal of Fluid Mechanics
Volume
814
Copyright Statement
© 2017 Cambridge University Press. This paper has been accepted for publication and will appear in a revised form, subsequent to peer-review and/or editorial input by Cambridge University Press.
Sponsor
Engineering & Physical Science Research Council (EPSRC)
Engineering & Physical Science Research Council (EPSRC)
Identifier
http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000395233600012&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=1ba7043ffcc86c417c072aa74d649202
Grant Number
EP/K041134/1
EP/L020564/1
Subjects
Science & Technology
Technology
Physical Sciences
Mechanics
Physics, Fluids & Plasmas
Physics
interfacial flows (free surface)
low-Reynolds-number flows
thin films
THIN LIQUID-FILMS
LINEAR-STABILITY
ELECTROHYDRODYNAMIC INSTABILITIES
DYNAMICS
SHEAR
EVOLUTION
RUPTURE
SYSTEM
FIELDS
BLOOD
01 Mathematical Sciences
09 Engineering
Fluids & Plasmas
Publication Status
Published