Page 112 - Tribology in Machine Design
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98   Tribology in machine design


     4.2. The concept of         Figure 4.1 represents a body A supporting a load W and free to slide on a
     friction angle              body B bounded by the stationary horizontal surface X—Y. Suppose the
                                 motion of A is produced by a horizontal force P so that the forces exerted by
                                 A on B are P and the load W. Conversely, the forces exerted by B on A are
                                 the frictional resistance F opposing motion and the normal reaction R.
                                 Then, at the instant when sliding begins, we have by definition



                                 We now combine F with /?, and P with, W, and then, since F = P and R = W,
                                 the inclination of the resultant force exerted by A and B, or vice versa, to the
                                 common normal NN is given by

     Figure 4.1
                                 The angle </> = tan  l  fi s called the angle of friction or more correctly the
                                 limiting angle of friction, since it represents the maximum possible value of 4>
                                 at the commencement of motion. To maintain motion at a constant
                                 velocity, K, the force P will be less than the value when sliding begins, and
                                 for lubricated surfaces such as a crosshead slipper block and guide, the
                                 minimum possible value of (/> will be determined by the relation



                                 In assessing a value for/, and also (f>, for a particular problem, careful
                                 distinction must be made between kinetic and static values. An example of
                                 dry friction in which the kinetic value is important is the brake block and
                                 drum shown schematically in Fig. 4.2. In this figure
                                        R = the normal force exerted by the block on the drum,
                                        F = the tangential friction force opposing motion of the drum,
                                        Q = F/sin(j)=the resultant of F and R,
     Figure 4.2                         D = the diameter of the brake drum.
                                 The retarding or braking is then given by



                                 The coefficient of friction, /, usually decreases with increasing sliding
                                 velocity, which suggests a change in the mechanism of lubrication. In the
                                 case of cast-iron blocks on steel tyres, the graphitic carbon in the cast-iron
                                 may give rise to adsorbed films of graphite which adhere to the surface with
                                 considerable tenacity. The same effect is produced by the addition of
                                 colloidal graphite to a lubricating oil and the films, once developed, are
                                 generally resistant to conditions of extreme pressure and temperature.


                                 4.2.1. Friction in slideways
                                 Figure 4.3 shows the slide rest or saddle of a lathe restrained by parallel
                                 guides G. A force F applied by the lead screw will tend to produce clockwise
                                 rotation of the moving element and, assuming a small side clearance,
     Figure 4.3                  rotation will be limited by contact with the guide surfaces at A and B. Let P
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