Page 29 - Tribology in Machine Design
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16   Tribology in machine design


                                 For most engineering materials this ratio is of the order of 0.2 and means
                                 that the friction coefficient may be of the same order of magnitude. In the
                                 case of clean metals, where the junction growth is most likely to take place,
                                 the adhesion component of friction may increase to about 10-100. The
                                 presence of any type of lubricant disrupting the formation of the adhesive
                                junction can dramatically reduce the magnitude of the adhesion com-
     Figure 2.2
                                 ponent of friction. This simple model can be supplemented by the surface
                                 energy of the contacting bodies. Then, the friction coefficient is given by (see
                                 Fig. 2.2)




                                        /
                                 where W 12 =yi+y 2 —Tia is the surface energy.
                                   Recent progress in fracture mechanics allows us to consider the fracture
                                 of an adhesive junction as a mode of failure due to crack propagation




                                 where <7 12 is the interfacial tensile strength, 6 C is the critical crack opening
                                 displacement, n is the work-hardening factor and H is the hardness.
                                   It is important to remember that such parameters as the interfacial shear
                                 strength or the surface energy characterize a given pair of materials in
                                contact rather than the single components involved.



     2.4. Friction due to        Ploughing occurs when two bodies in contact have different hardness. The
     ploughing                   asperities on the harder surface may penetrate into the softer surface and
                                 produce grooves on it, if there is relative motion. Because of ploughing a
                                 certain force is required to maintain motion. In certain circumstances this
                                 force may constitute a major component of the overall frictional force
                                 observed. There are two basic reasons for ploughing, namely, ploughing by
                                 surface asperities and ploughing by hard wear particles present in the
                                 contact zone (Fig. 2.3). The case of ploughing by the hard conical asperity is
                                 shown in Fig. 2.3(a), and the formula for estimating the coefficient of
                                 friction is as follows:




                                 Asperities on engineering surfaces seldom have an effective slope, given by
                                 0, exceeding 5 to 6; it follows, therefore, that the friction coefficient,
                                 according to eqn (2.9), should be of the order of 0.04. This is, of course, too
                                 low a value, mainly because the piling up of the material ahead of the
                                 moving asperity is neglected. Ploughing of a brittle material is inevitably
                                 associated with micro-cracking and, therefore, a model of the ploughing
                                 process based on fracture mechanics is in place. Material properties such as
     Figure 2.3                  fracture toughness, elastic modulus and hardness are used to estimate the
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