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8 Lubrication and efficiency of
                                     involute gears













     8.1. Introduction           Because it is assumed that the reader already has an understanding of the
                                 kinematics, stress analysis and the design of gearing, no further presen-
                                 tation of these topics will be given in this chapter. Instead, prominent
                                 attention will be given to lubrication and wear problems, because the
                                 successful operation of gears requires not only that the teeth will not break,
                                 but also that they will keep their precise geometry for many hours, even
                                 years of running. The second topic covered in this chapter is the efficiency of
                                 gears. It is customary to express the efficiencies of many power transmitting
                                 elements in terms of a coefficient of friction. A similar approach has been
                                 adopted here. In order to arrive at sensible solutions a number of
                                 simplifying assumptions are made. They are:
                                  (i) perfectly shaped and equally spaced involute teeth;
                                 (ii) a constant normal pressure at all times between the teeth in
                                     engagement;
                                 (hi) when two or more pairs of teeth carry the load simultaneously, the
                                     normal pressure is shared equally between them.

     8.2. Generalities of        If two parallel curved surfaces, such as the profiles of meshing spur gear-
     gear tribodesign            teeth, made of a truly rigid material, were pressed together they would make
                                 contact along a line, which implies that the area of contact would be zero,
                                 and the pressure infinite. No materials are rigid, however, so deformation of
                                 an elastic nature occurs, and a finite, though small area, carries the load.
                                 The case of two cylinders of uniform radii RI and R 2 was solved by Hertz. If
                                 we take the case of two steel cylinders for which v = 0.286 then the maximum
                                 compressive stress is given by





                                 where P is the compressive load per unit length of the cylinders and E is the
                                 equivalent Young modulus. If the radius of relative curvature R of the
                                 cylinders is defined as I//?! + 1/7?  2 then




                                 It should be noted that this stress is one of the three compressive stresses,
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