Page 31 - Tribology in Machine Design
P. 31

18  Tribology in machine design


                                 where A T is the real area of contact, r max denotes the ultimate shear strength
                                 of a material and T S is the average interfacial shear strength.

     2.6.  Energy dissipation    In a practical engineering situation all the friction mechanisms, discussed so
      during friction            far on an individual basis, interact with each other in a complicated way.
                                 Figure 2.5 is an attempt to visualize all the possible steps of friction-induced
                                 energy dissipations. In general, frictional work is dissipated at two different
                                 locations within the contact zone. The first location is the interfacial region
                                 characterized by high rates of energy dissipation and usually associated
                                 with an adhesion model of friction. The other one involves the bulk of the
                                 body and the larger volume of the material subjected to deformations.
                                 Because of that, the rates of energy dissipation are much lower. Energy
                                 dissipation during ploughing and asperity deformations takes place in this
                                 second location. It should be pointed out, however, that the distinction of
                                 two locations being completely independent of one another is artificial and
                                 serves the purpose of simplification of a very complex problem. The various
                                 processes depicted in Fig. 2.5 can be briefly characterized as follows:
                                  (i) plastic deformations and micro-cutting;
                                 (ii) viscoelastic deformations leading to fatigue cracking and tearing, and
                                     subsequently to subsurface excessive heating and damage;
                                 (iii) true sliding at the interface leading to excessive heating and thus
                                     creating the conditions favourable for chemical degradation
                                     (polymers);
                                 (iv) interfacial shear creating transferred films;
                                 (v) true sliding at the interface due to the propagation of Schallamach
                                     waves (elastomers).






















                       Figure 2.5


     2.7.  Friction under        Complex motion conditions arise when, for instance, linear sliding is
     complex motion              combined with the rotation of the contact area about its centre (Fig. 2.6).
     conditions                  Under such conditions, the frictional force in the direction of linear motion
   26   27   28   29   30   31   32   33   34   35   36