Finite amplitude cellular convection induced by surface tension

A non-linear analysis of cellular convection driven by surface tension in a semi-infinite liquid layer heated from below has been made. The purpose is to determine whether or not one can predict the emergence of the hexagonal flow pattern from the interaction of a certain large class of important disturbances. The principal conclusion is that, compared with gravity driven convection, there is generally a much greater band of imposed temperature difference associated with hexagonal convective patterns. Partial results for the more realistic assumption of finite depth support this conclusion.

[1]  A. Acrivos,et al.  Nature of the Neutral State in Surface‐Tension Driven Convection , 1966 .

[2]  K. A. Smith On convective instability induced by surface-tension gradients , 1966, Journal of Fluid Mechanics.

[3]  Andreas Acrivos,et al.  The effect of surface active agents on convection cells induced by surface tension , 1965 .

[4]  L. Segel The structure of non-linear cellular solutions to the Boussinesq equations , 1965, Journal of Fluid Mechanics.

[5]  L. Segel The non-linear interaction of a finite number of disturbances to a layer of fluid heated from below , 1965, Journal of Fluid Mechanics.

[6]  Donald A. Nield,et al.  Surface tension and buoyancy effects in cellular convection , 1964, Journal of Fluid Mechanics.

[7]  L. Scriven,et al.  On cellular convection driven by surface-tension gradients: effects of mean surface tension and surface viscosity , 1964, Journal of Fluid Mechanics.

[8]  L. Segel,et al.  On the question of the preferred mode in cellular thermal convection , 1962, Journal of Fluid Mechanics.

[9]  J. T. Stuart On the non-linear mechanics of wave disturbances in stable and unstable parallel flows Part 1. The basic behaviour in plane Poiseuille flow , 1960, Journal of Fluid Mechanics.

[10]  J. Watson,et al.  On the non-linear mechanics of wave disturbances in stable and unstable parallel flows Part 2. The development of a solution for plane Poiseuille flow and for plane Couette flow , 1960, Journal of Fluid Mechanics.

[11]  L. Scriven,et al.  The Marangoni Effects , 1960, Nature.

[12]  E. Palm On the tendency towards hexagonal cells in steady convection , 1960, Journal of Fluid Mechanics.

[13]  J. Pearson,et al.  On convection cells induced by surface tension , 1958, Journal of Fluid Mechanics.

[14]  M. Block,et al.  Surface Tension as the Cause of Bénard Cells and Surface Deformation in a Liquid Film , 1956, Nature.

[15]  H. Jeffreys THE SURFACE ELEVATION IN CELLULAR CONVECTION , 1951 .