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Basic principles of tribology  39


                                2.11.5. Adhesive wear equation
                                Theoretically, the volume of adhesive wear should strictly be a function of
                                the metal-metal contact area, A m, and the sliding distance. This hypothesis
                                is central to the model of adhesive wear. Thus, it can be written as



                                where k m is a dimensionless constant specific to the rubbing materials and
                                independent of any surface contaminants or lubricants.
                                  Expressing the real area of contact, A T, in terms of W and P and taking
                                into account the concept of fractional surface film defect, /?, eqn (2.83)
                                becomes



                                where Wis the load supported by the contacting asperities and P is the flow
                                pressure of the softer material in contact. Equation (2.84) contains a
                                parameter k m which characterizes the tendency of the contacting surfaces to
                                wear by the adhesive process, and a parameter P indicating the ability of the
                                lubricant to reduce the metal-metal contact area, and which is variable
                                between zero and one.
                                  Although it has been customary to employ the yield pressure, P, which is
                                obtained under static loading, the value under sliding will be less because of
                                the tangential stress. According to the criterion of plastic flow for a two-
                                dimensional body under combined normal and tangential stresses, yielding
                                of the friction junction will follow the expression


                                where P is now the flow pressure under combined stresses, S is the shear
                                strength, P m is the flow pressure under static load and a may be taken as 3.
                                An exact theoretical solution for a three-dimensional friction junction is not
                                known. In these circumstances however, the best approach is to assume the
                                two-dimensional junction.
                                  From friction theory



                                where F is the total frictional force. Thus




                                and eqn (2.84) becomes



                                Equation (2.87) now has the form of an expression for the adhesive wear of
                                lubricated contacts which considers the influence of tangential stresses on
                                the real area of contact. The values of W and ft can be calculated from the
                                equations presented and discussed earlier.
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