Page 30 - Tribology in Machine Design
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Basic principles of tribology  17


                                 coefficient of friction, which is given by




                                 where K k is the fracture toughness, E is the elastic modulus and H is the
                                 hardness.
                                   The ploughing due to the presence of hard wear particles in the contact
                                 zone has received quite a lot of attention because of its practical
                                 importance. It was found that the frictional force produced by ploughing is
                                 very sensitive to the ratio of the radius of curvature of the particle to the
                                 depth of penetration. The formula for estimating the coefficient of friction in
                                 this case has the following form:






     2.5 Friction due to         Mechanical energy is dissipated through the deformations of contacting
     deformation                 bodies produced during sliding. The usual technique in analysing the
                                 deformation of the single surface asperity is the slip-line field theory for a
                                 rigid, perfectly plastic material. A slip-line deformation model of friction,
                                 shown in Fig. 2.4, is based on a two-dimensional stress analysis of Prandtl.
                                 Three distinct regions of plastically deformed material may develop and, in
                                 Fig. 2.4, they are denoted ABE, BED and BDC. The flow shear stress of the
                                 material defines the maximum shear stress which can be developed in these
                                 regions. The coefficient of friction is given by the expression



     Figure 2.4
                                 where A = A(£; H) is the portion of plastically supported load, E is the elastic
                                 modulus and H is the hardness.
                                  The proportion of load supported by the plastically deformed regions
                                 and related, in a complicated way, to the ratio of the hardness to the elastic
                                modulus is an important parameter in this model. For completely plastic
                                asperity contact and an asperity slope of 45°, the coefficient of friction is 1.0.
                                 It decreases to 0.55 for an asperity slope approaching zero.
                                  Another approach to this problem is to assume that the frictional work
                                performed is equal to the work of the plastic deformation during steady-
                                state sliding. This energy-based plastic deformation model of friction gives
                                the following expression for the coefficient of friction:
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