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Non-Oberbeck-Boussinesq effects in strongly turbulent Rayleigh-Benard convection

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Title: Turbulent bubbly flow Author: Detlef Lohse Last modified by: PoF Created Date: 7/4/2000 3:32:24 PM Document presentation format: On-screen Show – PowerPoint PPT presentation

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Title: Non-Oberbeck-Boussinesq effects in strongly turbulent Rayleigh-Benard convection


1
Non-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
2
Oberbeck-Boussinesq dynamics
?, ?, ?, ?
3
Oberbeck-Boussinesq dynamics
Conflict of interest!
4
Large Ra regime
Non-Oberbeck-Boussinesq (NOB) effects?
5
Systematically explore NOB effects in water
small L9.5cm
medium L24.8cm
6
Effect of NOB top-down symmetry broken
OB
7
Notation
Control parameter
8
Characterization of (input) NOB effects
100 effect for ??, ? !
9
Characterizations of NOB effects(response of
system)
Measured
10
Experimental results on ?
about 15 effect
11
Experimental results on Nu
small cell
medium cell
large cell
1.5 effect (tiny decrease)
12
Experimental results on Re
NOB data No effect within 2 error bars
13
TheoryCalculation of Tc(and thus ?)
gtExtended Prandtl-Blasius BL theory
14
Extended velocity equation
15
Nondimensionalize
16
NOB version of Prandtl equation
17
Temperature equation
18
Non-dimensionalize
19
NOB version of temperature equation
How to determine ?c?
20
Coupling between top bottom BL
21
Temperature profiles
22
Center temperature Tc
23
Theory vs experiment ?
24
Nusselt number cannot yet be calculated
within extended Prandtl-Blasius BL theory
without additional assumptions
25
What can be answeredWhy is Nu so robust
towards NOB effects?
26
Heat flux conservation at top bottom
27
Robustness 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

28
Origin of NOB deviation for Nu
29
NuNOB/NuOB exp vs theory
30
Numerics2D NOB simulations
  • with Kazu Sugiyama and Enrico Calzavarini

31
Solve full Navier-Stokes eqs
with temperature and thus space dependent
material properties
32
Ra107
Water
OB
60
40
D 40K
20
Tm40oC
33
Central temperature vs D
BL theory
No convection
/K
Tm40oC
34
Ra108
Tm40oC
/K
35
Is F11 a general features?
  • gt try glycerol where the viscosity strongly
    depends on temperature

36
Ra107
Glycerol
OB
60
40
DT 40K
20
Tm40oC
37
Central temperature vs D
Ra104 (steady)
Tm40oC
/K
38
Tc vs ? for Ra107
/K
39
Nusselt 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
42
Summary
  • 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).
43
Acknowledgements
  • Financial support from
  • FOM

44
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45
Failure of Wu-Libchaber NOB theory
Wu Libchaber (PRA43, 2833 (1991)) introduce

and assume
46
Heat flux
47
Experimental Tc
48
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