• Aucun résultat trouvé

11 Vortex enhancement in streaming with viscoelastic fluids

N/A
N/A
Protected

Academic year: 2022

Partager "11 Vortex enhancement in streaming with viscoelastic fluids"

Copied!
1
0
0

Texte intégral

(1)

rencontre du non-lin´eaire 2021 1

Vortex enhancement in streaming with viscoelastic fluids

S. Amir Bahrani1,3, Maxime Costalonga1, Nicolas P´erinet4, Laurent Royon2 & Philippe Brunet1

1 Universit´e de Paris, CNRS, MSC, UMR 7057, F-75006, Paris, France

2 Universit´e de Paris, CNRS, LIED, UMR 8236, F-75006, Paris, France

3 IMT Lille Douai, Institut Mines T´el´ecom, Univ. Lille, Center for Energy and Environment, F-59000 Lille.

4 Departamento de F´ısica, Universidad de Chile, Casilla 487-3, Santiago, Chile.

amir.bahrani@imt-lille-douai.fr

Oscillations of immersed bodies are known to generate steady streaming flows, originating from Rey- nolds stresses within the viscous boundary layer in the vicinity of the object. This phenomenon is very similar to acoustic streaming generated by sound or ultrasound waves within a fluid. Streaming flows have applications in fluid homogenization and mixing especially in microfluidics, in heat transfer enhancement, in particle sorting or in fluid pumping. A typical situation is that of a cylinder oscillating perpendicularly to its axis, generating two pairs of counter-rotating vortices due to the transfer of vorticity from the inner boundary layer. Outer vortices can be observed far from the object as a result of convection of vorticity [1]. Here, we consider the situation of a viscoelastic fluid : by using PIV, we carry out an experimen- tal study of the streaming flow structure and magnitude varying both the amplitude and frequency of the cylinder oscillations. The fluid (HPAM + 1% NaCl) is chosen such that the relaxation time of its extensional viscosity is of the same order as the period of oscillations.

A systematic comparison with a purely Newtonian fluid has been carried out and results showed several qualitative differences. First, when elasticity is significant enough, we observe that the inner boundary layer vortices are much larger than for a Newtonian fluid of the same viscosity. This is generally associated to the disappearance of outer vortices. We propose that extensional viscosity is involved in the enlargement of inner vortices (Figure 1).

Figure 1.Enlargement of inner vortices within the secondary steady flows forf= 20 Hz.

Second, for strong enough forcing, the streaming flow moves away from the usual the four-vortices pattern. Indeed, a more complex structure can appear where each initial vortex splits into two smaller ones, showing a steady multiple vortices structure. To the best of our knowledge, these phenomena were unobserved so far.

R´ ef´ erences

1. S. A. Bahrani, N. P´erinet, M. Costalonga, L. Royon and P. Brunet, Exp. Fluids61, 91 (2020).

©Non Lin´eaire Publications, Avenue de l’Universit´e, BP 12, 76801 Saint- ´Etienne du Rouvray cedex

Références

Documents relatifs

Due to the discrete nature of the charge carriers, the current presents some fluctuations (noise) known as shot noise , which we aim to characterize here (not to be confused with

The theoretical study is developed using the approach of the inhomogeneous plane waves: the interface wave is thus regarded as a linear combination of one evanescent wave in the

We have examined the linear stability of a pulsed flow of a viscoelastic fluid in the Taylor-Couette geometry when the outer and the inner cylinders are oscillating in phase with

Finally, it can be noted that our conclusion are agree with the previous known results saying that the transverse mag- netic field has a stabilizing e ff ect on the plane Poiseuille

(a) A comparison between theoretical (——) and experimental (w) results: attenuation of the energy of the Stoneley–Scholte wave as a function of distance of propagation at the

In the cases examined, the azimuthal component of streaming flow driven by the equatorial Coriolis terms is everywhere retrograde, whereas that driven by Reynolds stresses may

Les diagrammes spatiotemporels de vitesses radiale pour différentes positions dans la direction axiale v r (z,t) montrent que le premier mode d’instabilité se manifeste sous la

represents an irrational number.. Hence, large partial quotients yield good rational approximations by truncating the continued fraction expansion just before the given