-
1
-
-
85037189079
-
-
The Rayleigh number is equal to (Formula presented) where Δ denotes the temperature difference between the bottom and top plates, (Formula presented) m the fluid layer thickness, (Formula presented) the acceleration of gravity, (Formula presented) the coefficient of thermal expansion, (Formula presented) the kinematic viscosity, and (Formula presented) the thermal diffusivity. Sometimes the Grashof number Gr=Ra/Pr is used instead, where Pr is the Prandtl number equal to Pr=ν/κ
-
The Rayleigh number is equal to (Formula presented) where Δ denotes the temperature difference between the bottom and top plates, (Formula presented) m the fluid layer thickness, (Formula presented) the acceleration of gravity, (Formula presented) the coefficient of thermal expansion, (Formula presented) the kinematic viscosity, and (Formula presented) the thermal diffusivity. Sometimes the Grashof number Gr=Ra/Pr is used instead, where Pr is the Prandtl number equal to Pr=ν/κ.
-
-
-
-
4
-
-
85037249806
-
-
S. Chandrasekhar Hydrodynamic and Hydromagnetic Stability (Dover, New York, 1961)
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S. Chandrasekhar Hydrodynamic and Hydromagnetic Stability (Dover, New York, 1961).
-
-
-
-
7
-
-
0005847902
-
-
K. Jirlow, Tellus 8, 252 (1956).
-
(1956)
Tellus
, vol.8
, pp. 252
-
-
Jirlow, K.1
-
10
-
-
85037177777
-
-
S. Cioni and J. Sommeria, Advances in Turbulence VII (Kluwer Academic, Dordrecht, 1998), pp. 419–423
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S. Cioni and J. Sommeria, Advances in Turbulence VII (Kluwer Academic, Dordrecht, 1998), pp. 419–423.
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-
-
-
11
-
-
85037251738
-
-
The Nusselt number is defined from the heat flux (Formula presented) across the convective cell (electrical heating power divided by the horizontal section 356 (Formula presented) as (Formula presented) where (Formula presented) is the volumetric heat capacity of mercury
-
The Nusselt number is defined from the heat flux (Formula presented) across the convective cell (electrical heating power divided by the horizontal section 356 (Formula presented) as (Formula presented) where (Formula presented) is the volumetric heat capacity of mercury.
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-
-
-
14
-
-
0000104481
-
-
T. Takeshita, T. Segawa, J. A. Glazier, and M. Sano, Phys. Rev. Lett. 76, 1465 (1996).
-
(1996)
Phys. Rev. Lett.
, vol.76
, pp. 1465
-
-
Takeshita, T.1
Segawa, T.2
Glazier, J.A.3
Sano, M.4
-
17
-
-
85037198553
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-
L. N. Howard in Proceedings of the 11th International Congress of Applied Mechanics, Munich, Germany (Springer, Berlin, 1966)
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L. N. Howard in Proceedings of the 11th International Congress of Applied Mechanics, Munich, Germany (Springer, Berlin, 1966).
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-
-
-
19
-
-
0024698819
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-
B. Castaing, G. Gunaratne, F. Heslot, L. Kadanoff, A. Libchaber, S. Thomae, X. Wu, S. Zaleski, and G. Zanetti, J. Fluid Mech. 204, 1 (1989).
-
(1989)
J. Fluid Mech.
, vol.204
, pp. 1
-
-
Castaing, B.1
Gunaratne, G.2
Heslot, F.3
Kadanoff, L.4
Libchaber, A.5
Thomae, S.6
Wu, X.7
Zaleski, S.8
Zanetti, G.9
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