Title: Non-Oberbeck-Boussinesq effects in strongly turbulent Rayleigh-Benard convection
1Non-Oberbeck-Boussinesq effects in strongly
turbulent Rayleigh-Benard convection
Guenter Ahlers, Eric Brown, Denis Funfschilling
Physics Department, Santa Barbara
F. Fontenele Araujo, Kazu Sugiyama, Enrico
Calzavarini, Siegfried Grossmann, Detlef Lohse
Physics of Fluids, University of Twente, The
Netherlands
2Oberbeck-Boussinesq dynamics
?, ?, ?, ?
3Oberbeck-Boussinesq dynamics
Conflict of interest!
4Large Ra regime
Non-Oberbeck-Boussinesq (NOB) effects?
5Systematically explore NOB effects in water
small L9.5cm
medium L24.8cm
6Effect of NOB top-down symmetry broken
OB
7Notation
Control parameter
8Characterization of (input) NOB effects
100 effect for ??, ? !
9Characterizations of NOB effects(response of
system)
Measured
10Experimental results on ?
about 15 effect
11Experimental results on Nu
small cell
medium cell
large cell
1.5 effect (tiny decrease)
12Experimental results on Re
NOB data No effect within 2 error bars
13TheoryCalculation of Tc(and thus ?)
gtExtended Prandtl-Blasius BL theory
14Extended velocity equation
15Nondimensionalize
16NOB version of Prandtl equation
17Temperature equation
18Non-dimensionalize
19NOB version of temperature equation
How to determine ?c?
20Coupling between top bottom BL
21Temperature profiles
22Center temperature Tc
23Theory vs experiment ?
24Nusselt number cannot yet be calculated
within extended Prandtl-Blasius BL theory
without additional assumptions
25What can be answeredWhy is Nu so robust
towards NOB effects?
26Heat flux conservation at top bottom
27Robustness of Nu
- Only sums of top bottom BL contributions
appear - NOB corrections to Nu depend on quadratic
contributions to NOB deviations of the
material parameters
28Origin of NOB deviation for Nu
29NuNOB/NuOB exp vs theory
30Numerics2D NOB simulations
- with Kazu Sugiyama and Enrico Calzavarini
31Solve full Navier-Stokes eqs
with temperature and thus space dependent
material properties
32Ra107
Water
OB
60
40
D 40K
20
Tm40oC
33Central temperature vs D
BL theory
No convection
/K
Tm40oC
34Ra108
Tm40oC
/K
35Is F11 a general features?
- gt try glycerol where the viscosity strongly
depends on temperature
36Ra107
Glycerol
OB
60
40
DT 40K
20
Tm40oC
37Central temperature vs D
Ra104 (steady)
Tm40oC
/K
38Tc vs ? for Ra107
/K
39Nusselt number deviation
40 F11 is no general features,
- but is incidental for water at Tm40oC and ?lt40K
- NOB-extended BL theory still works very
accurately for F2
41/K
42Summary
- 100 effect in ?, ?, 10 effect in ? (for
water) - 15 effect in Tc and
- less 2 effect in Nu and Re
- robustness theoretically understood
- NOB-extended BL theory works nicely for Tc and ?
- agreement with 2D numerics for water and
glycerol - in general, Nu cannot yet be theoretically
calculated
Ref. G. Ahlers et al., J. Fluid Mech., in press
(2006).
43Acknowledgements
- Financial support from
- FOM
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45Failure of Wu-Libchaber NOB theory
Wu Libchaber (PRA43, 2833 (1991)) introduce
and assume
46Heat flux
47Experimental Tc
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