Abstract
The unsteady flow of a viscous incompressible fluid in a circular
tube with an elastic
insertion is studied numerically. The deformation of the elastic membrane
is obtained
by the theory of finite elasticity whose equations are solved simultaneously
with the
fluid equations in the axisymmetric approximation. The elastic wall expands
outwards
due to the positive transmural pressure and represents an idealized model
for the
response of pathologies in large arteries.It is found that if either the fluid discharge or the reference pressure
are imposed
downstream of the insertion, the fluid–wall interaction develops
travelling waves along
the membrane whose period depends on membrane elasticity; these are unstable
in a
perfectly elastic membrane and are stabilized by viscoelasticity. In the
reversed system,
when the fluid discharge is imposed on the opposite side, the stable propagation
phenomenon remains the same because of symmetry arguments. Such arguments
do
not apply to the originally unstable behaviour. In this case, even when
the membrane
is perfectly elastic, propagation is damped and two natural fluctuations
appear in the
form of stationary waves. In all cases the resonance of the fluid–wall
interaction has
been analysed. Comparisons with previously observed phenomena and with
results
of analogous studies are discussed.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
26 articles.
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