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Basic principles of tribology  37


                                 Thus, eqn (2.72) becomes


                                 and finally


                                 Thus, the fractional film defect of the compounded lubricant is given by



                                 Following the same argument as in the case of the simple lubricant, it is
                                 possible to relate the fractional film defect for both (a) and (b) to the heat of
                                 adsorption, £ c,
                                   for additive (a)













                                 2.11.4.  Load sharing in lubricated contacts

                                 The adhesive wear of lubricated contacts, and in particular lubricated
                                 concentrated contacts, is now considered. The solution of the problem is
                                 based on partial elastohydrodynamic lubrication theory. In this theory,
                                 both the contacting asperities and the lubricating film contribute to
                                 supporting the load. Thus


                                where W c is the total load, W s is the load supported by the lubricating film
                                 and W is the load supported by the contacting asperities. Only part of the
                                total load, namely W, can contribute to the adhesive wear. In view of the
                                experimental results this assumption seems to be justified. Load W
                                supported by the contacting asperities results in the asperity pressure p,
                                given by


                                The total pressure resulting from the load W c is given by




                                Thus the ratio p/p c is given by


                                where Fi(d ea*) is a statistical function in the Greenwood-Williamson
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