Page 214 - Tribology in Machine Design
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Sliding-element bearings  199


                                 bearing. Consider the load to rotate at a uniform angular velocity o> p. When
                                 r is the radius of the shaft


                                 The case of a rotating load on a stationary bearing can be equated to that of
                                 a fixed load on a complete system which is rotated as a whole at velocity
      Figure 5.18
                                 — CJ P. Thus, the shaft velocity becomes o>i — o> p, the load vector is moving
                                 with speed (o p — co p=0 and the bearing velocity is 0 — co p= —co p. Then






                                 The problem can be expressed in terms of a general equation









                                 where R = ratio = (angular velocity of load)/(angular velocity of shaft).
                                 When R = % the load capacity is indicated as falling to zero, i.e. when the
                                 load is rotating at half the speed of the shaft.
                                   Experimental results show that under these circumstances, bearings
                                 operate at a dangerously high value of eccentricity, any lubricating film
                                 which may be present is attributed solely to secondary effect. Where the
                                 load operates at the speed of the shaft (a very common situation when
                                 machinery is out of balance), load-carrying capacity is the same as that for a
                                 steady load. As the frequency of a load increases so does the load-carrying
                                 capacity. Sometimes a hydrodynamic film exists between a non-rotating
                                 outer shell of a bearing and its housing. An out-of-balance load might, for
                                 example, be applied to the inner housing so that, although there was no
                                 relative lateral motion of the surfaces of the bearing outer shell and its
                                 housing, a rotating load would be applied thereto. Thus both coi and co 2 are
                                 zero so that the effective speed U becomes 2co pr. Thus a pressure film of
                                 twice the intensity of the case where the load is rotated with the shaft would
                                 be generated.


                                 5.5.6. Numerical example
                                 In a certain shaking device, an off-centre weight provides a centrifugal force
                                 of 26,000 N, rotating at 3600 r.p.m. This force is midway between the ends of
                                 the shaft, and it is shared equally by two bearings. Self-alignment of the
                                 bushing is provided by a spherical seat, plus loosely fitting splines to
                                 prevent rotation of the bushing about the axis of the shaft. The bearing is
                                 shown in Fig. 5.19. Oil of 10.3 mPas viscosity will be provided for
     Figure 5.19                 lubrication of the interior surfaces at I and the exterior surfaces at E. The
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