Stability of two-dimensional (2D) natural convection flows in air-filled differentially heated cavities: 2D/3D disturbances

被引:30
作者
Xin, Shihe [1 ,2 ,3 ]
Le Quere, Patrick [4 ]
机构
[1] Inst Natl Sci Appl, Cethil, UMR5008, F-69621 Villeurbanne, France
[2] Univ Lyon, F-69361 Lyon 07, France
[3] Univ Lyon 1, F-69622 Villeurbanne, France
[4] LIMSI CNRS, F-91403 Orsay, France
关键词
LINEAR-STABILITY; HOPF-BIFURCATION; PRANDTL NUMBER; CHAOS; UNSTEADINESS; TRANSITION;
D O I
10.1088/0169-5983/44/3/031419
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
Following our previous two-dimensional (2D) studies of flows in differentially heated cavities filled with air, we studied the stability of 2D natural convection flows in these cavities with respect to 3D periodic perturbations. The basis of the numerical methods is a time-stepping code using the Chebyshev spectral collocation method and the direct Uzawa method for velocity-pressure coupling. Newton's iteration, Arnoldi's method and the continuation method have been used in order to, respectively, compute the 2D steady-state base solution, estimate the leading eigenmodes of the Jacobian and perform linear stability analysis. Differentially heated air-filled cavities of aspect ratios from 1 to 7 were investigated. Neutral curves (Rayleigh number versus wave number) have been obtained. It turned out that only for aspect ratio 7, 3D stationary instability occurs at slightly higher Rayleigh numbers than the onset of 2D time-dependent flow and that for other aspect ratios 3D instability always takes place before 2D time-dependent flows. 3D unstable modes are stationary and anti-centro-symmetric. 3D nonlinear simulations revealed that the corresponding pitchfork bifurcations are supercritical and that 3D instability leads only to weak flow in the third direction. Further 3D computations are also performed at higher Rayleigh number in order to understand the effects of the weak 3D fluid motion on the onset of time-dependent flow. 3D flow structures are responsible for the onset of time-dependent flow for aspect ratios 1, 2 and 3, while for larger aspect ratios they do not alter the transition scenario, which was observed in the 2D cases and that vertical boundary layers become unstable to traveling waves.
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页数:15
相关论文
共 23 条
[1]   Three-dimensional centrifugal-flow instabilities in the lid-driven-cavity problem [J].
Albensoeder, S ;
Kuhlmann, HC ;
Rath, HJ .
PHYSICS OF FLUIDS, 2001, 13 (01) :121-135
[2]  
BERNARDI C, 1992, COLLECTION MATH APPL
[3]  
Boyd JP, 2000, CHEBYSHEV FOURIER SP
[4]  
Canuto C., 2012, Spectral Methods in Fluid Dynamics
[5]   Bifurcations and multiple solutions in a differentially heated cubic cavity [J].
de Gassowski, G ;
Xin, SH ;
Daube, O .
COMPTES RENDUS MECANIQUE, 2003, 331 (10) :705-711
[6]   On the approximation of the unsteady Navier-Stokes equations by finite element projection methods [J].
Guermond, JL ;
Quartapelle, L .
NUMERISCHE MATHEMATIK, 1998, 80 (02) :207-238
[7]   ACCURATE SOLUTION OF POISSONS EQUATION BY EXPANSION IN TSCHEBYSCHEFF POLYNOMIALS [J].
HAIDVOGEL, DB ;
ZANG, T .
JOURNAL OF COMPUTATIONAL PHYSICS, 1979, 30 (02) :167-180
[8]  
Keller H.B., 1977, Applications of Bifurcation Theory, P359
[9]   A direct (pseudo-spectral) solver of the 2D/3D Stokes problem: Transition to unsteadiness of natural-convection flow in a differentially heated cubical cavity [J].
Labrosse, G ;
Tric, E ;
Khallouf, H ;
Betrouni, M .
NUMERICAL HEAT TRANSFER PART B-FUNDAMENTALS, 1997, 31 (03) :261-276
[10]   From onset of unsteadiness to chaos in a differentially heated square cavity [J].
Le Quere, P ;
Behnia, M .
JOURNAL OF FLUID MECHANICS, 1998, 359 :81-107