The persistence of roughness between surfaces in static contact

When unworn rough metal surfaces are lightly pressed together the asperities of the softer surface in contact with the harder are commonly deformed plastically and support a contact pressure equal to their hardness. However, in heavily loaded contact conditions, in which the real areas of contact occupy a large proportion of the apparent area of contact, asperities can support contact pressures greater than their hardness: they are said to persist. Experimenters have disagreed about the size of the persistence effect and its cause: it has been ascribed to work hardening and to interaction between asperity deformation fields, a review of previous work suggests it depends on the type of surface finish. In this paper, which is limited to dry contact conditions, it is shown that surface texture has no practical effect on persistence. For a non-hardening material the contact pressure supportable by an asperity is proportional to its hardness but the constant of proportionality increases with the degree of contact between the surfaces. The increase is caused by asperity interaction in a manner predictable by plasticity mechanics. The same holds for a work-hardening material provided allowance is made for the increase of asperity hardness caused by its deformation. Asperities on a sand blasted surface, for example, may be strained 5% during their generation and up to a further 8% when pressed against another surface. Elastic deformation beneath the asperities also influences the degree of contact. This has not received due consideration in some earlier work.

[1]  D. Tabor Hardness of Metals , 1937, Nature.

[2]  J. Williamson,et al.  On the plastic contact of rough surfaces , 1972, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[3]  D. Whitehouse,et al.  The properties of random surfaces of significance in their contact , 1970, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[4]  Tarras Wanheim,et al.  Friction at high normal pressures , 1973 .

[5]  N. B. Demkin,et al.  Plastic contact under high normal pressure , 1975 .

[6]  K. Johnson,et al.  The correlation of indentation experiments , 1970 .

[7]  T. Childs,et al.  The persistence of asperities in indentation experiments , 1973 .

[8]  J. Greenwood,et al.  Contact of nominally flat surfaces , 1966, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[9]  N. Bay,et al.  Ra and the average effective strain of surface asperities deformed in metal-working processes , 1975 .

[10]  C. N. Baronet,et al.  Elastoplastic indentation of a half-space by an infinitely long rigid circular cylinder , 1971 .

[11]  Richard Timothy Hunt,et al.  Asperity persistence and the real area of contact between rough surfaces , 1972, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[12]  T. C. Chivers,et al.  The variation of real contact area between surfaces with contact pressure and material hardness , 1974 .

[13]  H. Blok Comments on the paper by R. Wilson , 1952, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[14]  The plastic contact between a rough and a flat surface , 1973 .

[15]  A. Moore,et al.  Deformation of metals in static and in sliding contact , 1948, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.