Abstract
Fine fibre immersed in different flows is ubiquitous. For a fibre in shear flows, most motion modes appear in the flow-gradient plane. Here the two-dimensional behaviours of an individual flexible flap in channel flows are studied. The nonlinear coupling of the fluid inertia (
$\textit {Re}$
), flexibility of the flap (
$K$
) and channel width (
$W$
) is discovered. Inside a wide channel (e.g.
$W=4$
), as
$K$
decreases, the flap adopts rigid motion, springy motion, snake turn and complex mode in sequence. It is found that the fluid inertia tends to straighten the flap. Moreover,
$\textit {Re}$
significantly affects the lateral equilibrium location
$y_{eq}$
, therefore affecting the local shear rate and the tumbling period
$T$
. For a rigid flap in a wide channel, when
$\textit {Re}$
exceeds a threshold, the flap stays inclined instead of tumbling. As
$\textit {Re}$
further increases, the flap adopts swinging mode. In addition, there is a scaling law between
$T$
and
$\textit {Re}$
. For the effect of
$K$
, through the analysis of the torque generated by surrounding fluid, we found that a smaller
$K$
slows down the tumbling of the flap even if
$y_{eq}$
is comparable. As
$W$
decreases, the wall confinement effect makes the flap easier to deform and closer to the centreline. The tumbling period would increase and the swinging mode would be more common. When
$W$
further decreases, the flaps are constrained to stay inclined, parabolic-like or one-end bending configurations moving along with the flow. Our study may shed some light on the behaviours of a free fibre in flows.
Funder
National Natural Science Foundation of China
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
4 articles.
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