Page 115 - Tribology in Machine Design
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Friction, lubrication and wear in lower kinematic pairs  101


                                 by a fixed stop S, and 4> is the angle of friction between the contact surfaces
                                 of B with A and S. Suppose the position of S is such that tilting of B occurs;
                                 the resultant reaction R± between the surfaces of A and B will then be
                                concentrated at the corner E. Let R 2 denote the resultant reaction between
                                 S and B, then, taking moments about E


                                The limiting case occurs when this couple is zero, i.e. when the line of action
                                 of ,R 2 passes through the intersection 0 of the lines of action of Wand R^.
     Figure 4.5                 The three forces are then in equilibrium and have no moment about any
                                point. Hence


                                 But



                                and


                                from which




                                Substituting these values of/?! and R 2 in eqn (4.6) gives











                                If a exceeds this value tilting will occur.
                                  The above problem can be solved graphically. The triangle of forces is
                                shown by OFE, and the limiting value of a can be determined directly by
                                drawing, since the line of action of R 2 then passes through O. For the
                                particular case when the stop S is regarded as frictionless, SF will be
                                horizontal, so that









                                  Now suppose that A is replaced by the inclined plane or wedge and that B
                                moves in parallel guides. The angle of friction is assumed to be the same at
                                all rubbing surfaces. The system, shown in Fig. 4.6, is so proportioned that,
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