2006
DOI: 10.1016/j.surfrep.2006.04.001
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Contact mechanics for randomly rough surfaces

Abstract: When two solids are squeezed together they will in general not make atomic contact everywhere within the nominal (or apparent) contact area. This fact has huge practical implications and must be considered in many technological applications. In this paper I briefly review basic theories of contact mechanics. I consider in detail a recently developed contact mechanics theory. I derive boundary conditions for the stress probability distribution function for elastic, elastoplastic and adhesive contact between sol… Show more

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Cited by 635 publications
(586 citation statements)
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“…For elastic solids with randomly rough surfaces, and assuming non-adhesive contact, the area of real contact A is given by [19][20][21][22] …”
Section: System C20mentioning
confidence: 99%
“…For elastic solids with randomly rough surfaces, and assuming non-adhesive contact, the area of real contact A is given by [19][20][21][22] …”
Section: System C20mentioning
confidence: 99%
“…This is an important result as U el u is relevant for many important applications. Theories show that, for low squeezing pressure, the area of real contact A varies linearly with the squeezing force pA 0 and that the interfacial stress distribution and the size distribution of contact spots are independent of the squeezing pressure [12,13]. That is, with increasing p, existing contact areas grow and new contact areas form in such a way that, in the thermodynamic limit (infinite-sized system), the quantities referred to above remain unchanged.…”
mentioning
confidence: 99%
“…The Degree of surface deformation is evaluated on the basis of function, power spectral density C(q) [4] and used in the analysis of surface stresses Eq(1):…”
Section: Results Of the Distribution Of Surface Potentialsmentioning
confidence: 99%