Page 253 - Cam Design Handbook
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THB8  9/19/03  7:25 PM  Page 241

                                    CAM MECHANISM FORCES                   241



                           A


                                 m
                                               P
                              a
                                 q           r
                                                  f
                                                         b
                                     d                        C
                              A o           B o       y
                                             x

                          FIGURE  8.19.  Schematic  sketch  of  the  mechanism  for  the
                          purpose of writing the design equations.


            new  mechanism.  Here,  we  use  a  more  appropriately  defined  index  of  transmission  as
            shown in Fig. 8.19. The torque exerted on the output member, the cam, is the moment due
            to the contact force between the roller and the cam, which acts along the common normal.
            The moment arm is given by r, which is the perpendicular distance to the common normal
            from the cam pivot. The higher the value of r is, the better the transmission and vice versa.
            As shown the nondimensionalized r is a convenient measure of transmission for the mech-
            anism considered here. The ratio (r/d) is the nondimensional transmission index for this
            mechanism.
               As shown in Fig. 8.19, point C is the instantaneous center of the roller crank and the
            cam. Therefore, this point has the same velocity on both the cam and the roller crank. This
            leads to the following relationship:
                                            df  x
                                         n =  =  .                        (8.20)
                                            dq  y
            Further, since x = y + d, Eq. (8.20) can be rewritten as

                                          1  n - 1
                                           =    .                         (8.21)
                                          y   d
            Now, applying the sine rule to the triangle A 0 AC of Fig. 8.19, we get
                                      (
                                    sin 180∞- q  - ) b  sin b
                                                 =                        (8.22)
                                          x         a
            which, after eliminating x, can be simplified to
                                                   yd
                                                    +
                                      q
                                    sin cotb +  cosq =  .                 (8.23)
                                                    a
            From the right-angled triangle B 0PC,
                                                   y
                                         y  2  - r  2  Ê ˆ  2
                                  cotb =       =      -1 .                (8.24)
                                           r     Ë ¯
                                                   r
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