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14 Hydrodynamic bistability in the VKS experiment: evidence of two dynamo branches

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Hydrodynamic bistability in the VKS experiment : evidence of two dynamo branches

S. Miralles1 & VKS collaboration1,2,3

1 Laboratoire de Physique ´Ecole Normale Sup´erieure de Lyon, UMR CNRS 5672, 46, All´ee d’Italie 69007 Lyon

2 Laboratoire de Physique Statistique ´Ecole Normale Sup´erieure de Paris, UMR 8550, 24 rue Lhomond 75231 Paris Cedex 05

3 SPHYNX Syst`emes Physiques Hors´equilibre, hYdrodynamique, ´eNergie et compleXite, CNRS/MPPU/URA 2464, Bat 772, Orme des Merisiers CEA Saclay

sophie.miralles@ens-lyon.fr

Self-sustained magnetic field has been observed in the Von K´arm´an Sodium experiment, where a highly turbulent liquid flow is created by the counter rotation of soft iron impellers ([1]). The high level of turbulence, the presence of a shear layer and of helicity make Von K´arm´an flows good candidates for fluid dynamo generation. These flows have been extensively studied in water experiments, where hydro- dynamic bifurcations for asymmetric driving were observed with possible multistability between these different flows ([2]).

The link between some bifurcations observed on the dynamo magnetic field and hydrodynamics bifurca- tions is still open ; although clues linking them has been reported ([3]).

Recently, a modification of the setup where one of the impeller has been replaced by a stainless steel propeller (aiming at reversing the poloidal flow and creating a s1t2 flow according to the Dudley and James classification).

We denoteF1 the rotation rate of the impeller and F2 the propeller’s one. A hydrodynamic bifurcation has been observed when the driving is strongly asymmetric, keepingF1constant and increasingF2. When the parameterθ=F2−F1/F1+F2(indicating the asymmetry of the driving) increases, the flow suddenly bifurcates forθ= 0.54 into a state close to as1t1 flow with only one poloidal cell and one toroidal cell.

Then, when θdecreases again, we observe an hysteretic behavior of the flow. It recovers its initial state only atθ= 0.43.

The striking fact is that this hydrodynamic bistability is associated to a bistability of the magnetic field.

The dynamo magnetic field displays a high amplitude axial dipole on one branch whereas when the flow has bifurcated, the magnetic field is a stationary low amplitude dynamo.

We will study in details the hydrodynamic bifurcation and the associated change on the magnetic field by local and global measurements and show that for two different flows with different level of fluctuations, it exists two stationary dynamo branches with different thresholds.

R´ ef´ erences

1. R. Monchaux et al., Generation of a Magnetic Field by Dynamo Action in a Turbulent Flow of Liquid SodiumPhys. Review Letters,98, (2007).

2. F. Ravelet et al., Multistability and memory effect in a highly turbulent flow : Experimental evidence for a global bifurcationPhys. Review Letters,93, (2004).

3. M. Berhanu et al., Bistability between a stationary and a oscillatory dynamo in a turbulent flow of liquid sodiumJ. of Fluid Mech.,641, (2009).

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