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- W81337327 abstract "When an horizontal layer of pure fluid, depth of which is d, is submitted to a temperature gradient ΔT, as shown on Fig.1, motion sets in, when ΔT exceeds a critical value ΔTc. The properties of this motion are related to the Rayleigh number $${R_{a}} = frac{{partial g.Delta T{d^{3}}}}{{vk}} ]$$where α, ν and κ are respectively the volumic expansion coefficient, the cinematic viscosity and the thermal diffusivity of the fluid: the Rayleigh number takes into account the different mechanisms involved in the convective motion: buoyancy forces, viscous damping, and thermal relaxation, according to the fact that, here, we are dealing only with fluid layers under rigid-rigid horizontal boundaries. (In this case, Rac = 1707)." @default.
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- W81337327 date "1979-01-01" @default.
- W81337327 modified "2023-09-24" @default.
- W81337327 title "Velocity Field in the Rayleigh-Benard Instability: Transitions to Turbulence" @default.
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- W81337327 doi "https://doi.org/10.1007/978-3-642-67262-0_17" @default.
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