Page 129 - Dynamics of Mechanical Systems
P. 129

0593_C04*_fm  Page 110  Monday, May 6, 2002  2:06 PM





                       110                                                 Dynamics of Mechanical Systems


                       and

                                                                  rψ
                                                        C
                                                              C
                                                      V = 0,  a = ˙  2 n                      (4.12.10)
                                                                      3
                        Observe that even though the velocity of the contact point is zero, its acceleration is
                       not zero.






                       4.13 A Conical Thrust Bearing
                       As another example illustrating rolling kinematics, consider a thrust bearing* consisting
                       of a cylindrical shaft with a conical end rolling on four spheres (or balls) as depicted in
                       Figure 4.13.1. Let the spheres roll in a cylindrical race R as shown. Let S refer to the shaft,
                       and let B refer to a typical ball. Let C , C , and C  be contact points between S and B and
                                                        1  2      3
                       between B and R, as shown. Let G be the center of B. Let θ be the half-angle of the conical
                       end of S, and let a be the distance between G and the axis of S. Let r be the radius of B.
                        As noted above, B rolls on both R and S. Suppose we desire B to have pure rolling on S
                       (see Eq. (4.11.2)). One might ask if there is a relationship between a, r, and θ that will
                       produce pure rolling between B and S while maintaining rolling between B and R. To
                       answer this question, consider an analysis of the kinematics of  B and  S: Figure 4.13.2
                       shows an enlarged view of the contact region between B and S. Let n , n , and n  be a set
                                                                                    1  2      3
                       of mutually perpendicular unit vectors such that n  is parallel to the axis of S and n  is
                                                                     2                             1
                       parallel to a line passing through G and C  and intersecting the axis of S. Let n  be a unit
                                                            3                                ⊥
                       vector parallel to GC and thus normal to the contacting surfaces of B and S at C . Let n
                                                                                              1      
                       be perpendicular to n  and n . Thus, n  is parallel to a cone element passing through C .
                                                         
                                          ⊥
                                                                                                     1
                                                 3
                        To study the kinematics and especially the rolling, it is helpful to first obtain expressions
                       for the angular velocities of S and B: Let Ω be the angular speed of the shaft S as indicated
                       in Figure 4.13.2. Then, the angular velocity of S in the reference frame R of the race is:
                                                          R  S
                                                           ωω= Ωn                              (4.13.1)
                                                                  2
                                                      S                 Ω                    S
                                                                                n  ⊥
                                                                                            n
                                                                                                  n
                                                                                                  2
                                                                                            B
                                                                        b
                                 θ                  B
                                             C  1                            θ     C  1            n
                                                                                                     1
                                                                                     G
                              r                   G                                      C
                                                        C                                 2        n
                                                         2                                          3
                       R                                                            C  3
                                   a              C  3                       a                R
                       FIGURE 4.13.1                              FIGURE 4.13.2
                       A conical thrust ball bearing.             Ball and shaft geometry.

                       * This problem is discussed by Kane (4.1, 4.2) and Cabannes (4.5); see also Ramsey (4.6).
   124   125   126   127   128   129   130   131   132   133   134