Page 266 - Tribology in Machine Design
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Rolling-contact bearings  251

                                  Torque, M gr, increases with an increase in contact angle a and attains a
                                 maximum value when y. = n/2. Thrust bearings, for example, have such an
                                 angle. Radial bearings are characterized by a =0, so that M gr =0. In order
                                 to avoid gyroscopic spin of the balls it is necessary to satisfy the inequality


                                where P is the axial load. The effect of gyroscopic spin is especially
                                 noticeable in radial thrust bearings.



                                 7.2.3. Friction torque due to elastic hysteresis
                                 The energy losses due to elastic hysteresis in the material of the bearing can
                                 be determined, assuming that during the loading cycle a specific quantity of
                                 kinetic energy is expended. Friction torque caused by elastic hysteresis has
                                 been sufficiently studied for the case of slow-running bearings. In the case of
                                 high-speed running, however, large centrifugal forces arise and they create
                                 an additional load. Hence, in all the expressions given below, friction torque
                                 M must be treated as a function of rotational speed.
                                   When the ball rolls along the raceway, the Hertz contact ellipse is formed
                                 between them as shown in Fig. 7.4. The energy developed during the rolling
                                 of the body about one point of the raceway is proportional to the load and
                                 to the magnitude of deformation. Contact time, f, of the rolling body with
     Figure 7.4
                                 the raceway is directly proportional to the extent of the contact surface in
                                 the direction of motion 2b and inversely proportional to the circumferential
                                 velocity, rco (see Fig. 7.5), thus




                                 The energy losses during the contact of the rolling body with one point of
     Figure 7.5                  the raceway are


                                 where P is the load and d denotes the associated deformation.
                                   According to the Hertz theory, the deformation for point contact is given
                                 by


                                 where Up is the sum of the reciprocal of the principal radii of curvature, i.e.



                                 here PI and p 2 are the reciprocals of the principal radii of curvature of the
                                 bodies at the point of contact and K is a coefficient depending on the
                                 function F(p) defined as
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