The high Rayleigh number (Ra) axisymmetric convection regimes of Pr=1 pure and (Le=0.1, Ψ=0.2) binary liquids are numerically investigated and compared. The fluids are enclosed in a vertical cylinder of aspect ratio heightradius=2 and heated from below, with either no-slip or free-slip kinematic lateral boundary conditions. Branches of solutions and transitions between states that occur as Ra is varied up to O(105) are given, along with a description of the encountered bifurcations. When a free-slip condition is imposed along the circumference of the cell, pure fluid and binary liquid stationary flows are found to become identical at high Ra, an often reported feature. When the lateral boundary condition is set to no-slip, the high Ra steady flows of pure and binary liquid, although very similar, undergo different bifurcations. This is related with a locally quasiquiescent region present in both cases, the stability of which controls the flow regime in the whole fluid layer. A branch of resulting oscillatory states thus does not appear in the bifurcation diagram of the binary liquid.

1.
E.
Bodenschatz
,
W.
Pesch
, and
G.
Ahlers
, “
Recent developments in Rayleigh–Bénard convection
,”
Annu. Rev. Fluid Mech.
32
,
709
(
2000
).
2.
J. K.
Platten
and
J. C.
Legros
,
Convection in Liquids
(
Springer
, Berlin,
1984
).
3.
M. C.
Cross
and
P. C.
Hohenberg
, “
Pattern formation outside of equilibrium
,”
Rev. Mod. Phys.
65
,
851
(
1993
).
4.
M.
Lücke
,
W.
Barten
,
P.
Büchel
,
C.
Fütterer
,
C.
Hollinger
, and
Ch.
Jung
, “
Pattern formation in binary fluid convection and in systems with throughflow
,” in
Evolution of Structures in Dissipative Continuous Systems
, edited by
F. H.
Busse
and
S. C.
Müller
(
Springer
, Berlin,
1998
).
5.
P.
Kolodner
,
S.
Slimani
,
N.
Aubry
, and
R.
Lima
, “
Characterization of dispersive chaos and related states of binary-fluid convection
,”
Physica D
85
,
165
(
1995
).
6.
W.
Barten
,
M.
Lücke
,
W.
Hort
, and
M.
Kamps
, “
Convection in binary fluid mixture. I. Extended traveling-wave and stationary states
,”
Phys. Rev. E
51
,
5636
(
1995
).
7.
D.
Bensimon
,
A.
Pumir
, and
B. I.
Shraiman
, “
Nonlinear theory of traveling wave convection in binary mixtures
,”
J. Phys. (France)
50
,
3089
(
1989
).
8.
H.
Touiri
,
J. K.
Platten
, and
G.
Chavepeyer
, “
Effect of the separation ratio on the transition between travelling waves and steady convection in the two-component Rayleigh–Bénard problem
,”
Eur. J. Mech. B/Fluids
11
,
2078
(
1996
).
9.
A.
La Porta
,
K. D.
Eaton
, and
C. M.
Surko
, “
Transition between curved and angular textures in binary fluid convection
,”
Phys. Rev. E
53
,
570
(
1996
).
10.
E.
Millour
,
G.
Labrosse
, and
E.
Tric
, “
Sensitivity of binary liquid thermal convection to confinement
,”
Phys. Fluids
15
,
2791
(
2003
).
11.
M.
Wanschura
,
H. C.
Kuhlmann
, and
H. J.
Rath
, “
Three-dimensional instability of axisymmetric buoyant convection in cylinders heated from below
,”
J. Fluid Mech.
326
,
399
(
1996
).
12.
G. S.
Charlson
and
R. L.
Sani
, “
On thermoconvective instability in a bounded cylindrical fluid layer
,”
Int. J. Heat Mass Transfer
14
,
2157
(
1970
).
13.
L. S.
Tuckerman
and
D.
Barkley
, “
Global bifurcation to traveling waves in axisymmetric convection
,”
Phys. Rev. Lett.
61
,
408
(
1988
).
14.
D.
Barkley
and
L.
Tuckerman
, “
Traveling waves in axisymmetric convection: the role of sidewall conductivity
,”
Physica D
37
,
288
(
1989
).
15.
C. M.
Aegerter
and
C. M.
Surko
, “
Effects of lateral boundaries on traveling-waves dynamics in binary fluid convection
,”
Phys. Rev. E
63
,
046301
(
2001
).
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