Abstract

Professor Simon has raised a very interesting point about the difference between rolling and sliding friction. In essence his query is concerned with the relation between the work done in creating a new surface of a solid and the free surface energy gained. This equivalence is valid for liquids and also applies as a first approximation to brittle solids with well-defined cleavage planes which show little capacity for plastic flow. Thus Obreimoff (1930) has determined the surface tension of mica from the work required to strip off a mica flake. Unfortunately, this concept cannot be applied to solids which undergo appreciable plastic flow before rupture occurs. It is not, of course, that plastic solids disobey the fundamental laws of thermodynamics, but that, in the formation of new surfaces by rupture, by far the greater part of the energy is dissipated in deforming the solid; the surface energy is only a small part of the whole.

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