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Journal ArticleDOI

On convection cells induced by surface tension

J. R. A. Pearson
- 01 Sep 1958 - 
- Vol. 4, Iss: 05, pp 489-500
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TLDR
In this paper, a mechanism was proposed by which cellular convective motion of the type observed by H. Benard, which hitherto has been attributed to the action of buoyancy forces, can also be induced by surface tension forces.
Abstract
A mechanism is proposed by which cellular convective motion of the type observed by H. Benard, which hitherto has been attributed to the action of buoyancy forces, can also be induced by surface tension forces. Thus when a thin layer of fluid is heated from below, the temperature gradient is such that small variations in the surface temperature lead to surface tractions which cause the fluid to flow and thereby tend to maintain the original temperature variations. A small disturbance analysis, analogous to that carried out by Rayleigh and others for unstable density gradients, leads to a dimensionless number B which expresses the ratio of surface tension to viscous forces, and which must attain a certain minimum critical value for instability to occur. The results obtained are then applied to the original cells described by Benard, and to the case of drying paint films. It is concluded that surface tension forces are responsible for cellular motion in many such cases where the criteria given in terms of buoyancy forces would not allow of instability.

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References
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Journal ArticleDOI

On Maintained Convective Motion in a Fluid Heated from below

TL;DR: In this article, the stability in viscous liquid of a steady regime in which the temperature decreases with uniform gradient between a lower horizontal surface which is heated and an upper horizontal surface that is cooled is examined.
Journal ArticleDOI

Some Cases of Instability in Fluid Motion

TL;DR: In this paper, the authors obtained a numerical solution of some problems concerning the stability of a layer of incompressible fluid when the temperature decreases upwards, and the results depended on the solution of the sixth-order differential equation (d 2/d ζ2 -a 2)3 Z = -λ a 2Z.
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