Page 82 - Cam Design Handbook
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THB3  8/15/03  12:58 PM  Page 70

          70                       CAM DESIGN HANDBOOK

          Substituting to find the velocity

                                 v = 22 5.  (07767.  ) =17 5.  ips
                                  A
                                 v = 93 3.  (07767.  ) = 72 5.  ips
                                  B
                                 v = maximum velocity
                                  T
                                   =  v + D v
                                     B    B to  T
                                        +
                                             =
                                   = 72 5 17 5 900 ips
                                           .
                                      .
          Also, the maximum acceleration
                                      (
                               A = 31700 7767 ) = 2460 in sec 2
                                        .
                                A
          The curves may now be plotted in Fig. 3.6b. If they were to be compared with a trape-
          zoidal acceleration curve, we would find that this curve has a slightly lower maximum
          acceleration and the advantage of lower required cutting accuracy in the initial and final
          rise portions. Also, the vibrations induced at high speeds should be slightly smaller than
          those of the trapezoidal curve.


          3.6 SKEWED MODIFIED TRAPEZOIDAL CURVE

          Occasionally, the follower requires a particular velocity and acceleration at some critical
          points  in  the  machine  motion.  This  can  be  accomplished  by  skewing  the  acceleration
          profile as seen in Fig. 3.7. Neklutin (1969) has treated the modified trapezoidal curve with
          unequal periods of acceleration, positive and negative. Ragsdell and Gilkey (1969) have
          related the skewed acceleration to a correspondingly symmetrical one. Before skewing is
          considered, the follower rise h and angle b have been determined and will be considered
          as constants.
             Let b 1 and b 2 be the periods during positive and negative acceleration, respectively,
                   b
          and let  p =  1  be the skew ratio (Fig. 3.7). Thus
                   b
                    2
                                       b +  b =  b
                                        1   2
                                       h  + h  = h.
                                        1  2
          The velocity match at the transition point that
                                      (y ¢ ) = (y ¢ )
                                       max 1  max 2
          Substituting and equating from Eq. (3.9)
                                       2h 1  =  2h 2
                                       b 1  b  2
                                             p
                                      \  b =   b
                                         1
                                             +
                                            1 p                         (3.10)
                                             p
                                        h =     h
                                         1
                                            1 p
                                             +
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