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First transitions in circular Couette flow with axial stratification

 

作者: Bach Lien Hua,   Sylvie Le Gentil,   Paolo Orlandi,  

 

期刊: Physics of Fluids  (AIP Available online 1997)
卷期: Volume 9, issue 2  

页码: 365-375

 

ISSN:1070-6631

 

年代: 1997

 

DOI:10.1063/1.869237

 

出版商: AIP

 

数据来源: AIP

 

摘要:

The first flow regimes which have been observed experimentally for a circular Couette flow with a stable, axial stratification in density are investigated through direct numerical simulations of the three-dimensional Navier-Stokes equations for a Boussinesq fluid. The setup of two concentric cylinders has a nondimensional gap width of&egr;=(b−a)/a=0.289;the outer cylinder is fixed and the stratification in density in the axial direction is linear. The main effect of an axial density stratification is to reduce the height of the Taylor vortices and to cause the formation of density layers of small aspect ratio. For large enough Prandtl number, the primary bifurcation from circular Couette flow is found to be axisymmetric and of Hopf-type in the direct numerical simulations. An analytical solution for onset of instability and slightly different boundary conditions from the experimental ones agrees within 0.6&percent; with numerical simulations at a Prandtl number of 700. The experimental flow regimes with well-defined density layers are well reproduced by the numerical simulations in the appropriate range of relative Reynolds numberRe/Rec1,whereRec1denotes the critical Reynolds number for the primary bifurcation from circular Couette flow. However, the increase of axial scale withRe/Rec1is found to be continuous, whereas it is quantized in the laboratory experiments. Numerical results reveal that the first two transitions between the flow regimes are primarily due to the temporal behavior of the axially symmetric part of the flow. Onset of nonaxisymmetric motions appears at the sameRe/Rec1≈1.18as in the homogeneous fluid case at the same&eegr;=a/b.Stratification precludes large axial displacements and the azimuthal modes patterns have a quite distinct appearance from the homogeneous wavy modes. At large enough Re, a destabilization of the jet-like outflow between pairs of vortices causes the suppression of the density front which is located at the same axial height. This nonaxisymmetric flow regime presents common features with the wavy outflow boundary (WOB) pattern, which is commonly observed in the homogeneous Couette-Taylor case. ©1997 American Institute of Physics.

 

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