Eur. Phys. J. B 45, 555-560 (2005)
https://doi.org/10.1140/epjb/e2005-00211-7

Scaling in convective evaporation and sidewall boundary layer

Laboratoire Hydrogéochimie et Études de sites, Commissariat à l'Énergie Atomique, B.P. 12, 91680 Bruyères-le-Châtel, France

Corresponding author: ^a perrier@ipgp.jussieu.fr

Received: 23 November 2004
Revised: 8 March 2005
Published online: 13 July 2005

Abstract

Turbulent convection at aspect ratios from 0.06 to 2 is investigated in the laboratory with evaporation experiments from vertical cylinders having different diameters and liquid levels. With alcohol, only diffusive evaporation takes place. With water, for small diameters, evaporation proceeds by diffusion whereas convective evaporation develops when the diameter is increased. This onset can be effectively interpreted in terms of a viscous sidewall boundary layer, whose thickness δ varies with respect to the available height h according to δ/h = 3.4 Ra versus Rayleigh number Ra. The Sherwood number Sh, analog of the Nusselt number, exhibits a power law variation Sh = 0.6 Ra for Ra varying from 10⁴ to . The scaling observed in this case of an open boundary is thus similar to the scaling measured in confined Rayleigh-Bénard convection.