Page 378 - Cam Design Handbook
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THB12  9/19/03  7:34 PM  Page 366

          366                      CAM DESIGN HANDBOOK

          be less than one-thousandth of the amplitude of the first harmonic and thus are unlikely
          to cause major problems. These observations also imply that accurate control of the high-
          order derivatives is not critical in controlling system vibration.
             With the open-track cam-follower system we may have a condition called jump or
          bounce. It is a transient condition that occurs with high-speed and highly flexible systems.
          With jump, the cam and the follower separate owing to excessively unbalanced forces
          exceeding the spring force during the period of negative acceleration. This is undesirable
          since the fundamental function of the cam-follower system, the constraint and control of
          follower motion, is not maintained. Also related are short life of the cam flank surface,
          high noise, vibrations, and poor action.
             Figure 12.5 depicts high-speed, highly flexible cam mechanism running at 2100rpm
          with b 1 = 27 degrees and a follower natural frequency of 42,000 cycles per minute. Figure
          12.5 shows the asymmetrical cam acceleration curve with the positive acceleration period
          of the 4-5-6-7 polynomial. Superimposed is the natural follower acceleration for various
          values of the frequency ratio. Also shown is the compression spring curve below the neg-
          ative acceleration values to maintain constraint of the follower on the cam. Jump occurs
          when  the  response  curve  falls  below  the  spring  curve. Turkish  (1953)  in  his  excellent
          article verifies this by tests. We see that jump becomes more predominant with smaller
          values of n (Baratta and Bluhm, 1954).
             A direct  approach  for  establishing  the  minimum  allowable  value  of  n to  prevent
          jump is shown by Karman and Biot (1940). Increasing the spring load is a poor way to
          eliminate  jump,  since  greater  surface  stresses  and  shorter  life  result. A design  method


                        12
                               n = 1       Actual response of follower
                               1
                        10   n = 1 / 2     with damping
                         8   n = 2         Cam acceleration curve,4-5-6-7
                         6
                      Acceleration in./degree 2  ¥ 10 2  -2   Cam angle q
                                                          Polynomial
                         4
                         2
                         0



                        -4

                        -6
                                               Jump    Spring curve
                        -8             b 1     Without damping
                       -10

                       -12
                     FIGURE  12.5.  Jump  phenomenon—transient  response  of  follower
                     (cam  rotates  2100rpm,  b 1 = 27  degrees,  follower  natural  frequency  =
                     42,000 cycles/min).
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