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THB4  8/15/03  1:01 PM  Page 104

          104                      CAM DESIGN HANDBOOK





                              y"



                                Cam angle q             b






                            FIGURE 4.10.  Gutman’s [1961] 1-3 harmonic
                            acceleration curve.

             Similarly, if we retain the first three terms in the Fourier series expansion of the dis-
          placement of the parabolic curve, the equation of Gutman’s fifth-order harmonic curve can
          be obtained.


          Freudenstein 1-3 Harmonic Curve (Freudenstein, 1960)
                                hq   h Ê 27  2 pq  1   6 pq  ˆ
                             y =   -   Á  sin   +   sin   ˜
                                    b  2 p  Ë 28  b  84  b  ¯
                                h  Ê  27  2 pq  1   6 pq  ˆ
                             y ¢ =  Á1 -  cos  -  cos   ˜
                                   b  Ë  28  b  28   b  ¯
                                2p h  Ê 27  2pq  3  6pq  ˆ
                            y ¢¢ =  Á  sin   +   sin  ˜
                                   b  2  Ë 28  b  28  b  ¯

                                4p  2 h  Ê 27  2pq  9  6pq  ˆ
                            y ¢¢¢ =  Á  cos   +   cos   ˜               (4.12)
                                  b  3  Ë 28  b  28   b  ¯
          In agreement with the foregoing design factors stated, Freudenstein’s 1-3 harmonic curve
          has a maximum acceleration of about 135 percent of the acceleration of the parabolic
          curve, or 85 percent of the acceleration of the cycloidal curve.


          Freudenstein 1-3-5 Harmonic Curve (Freudenstein, 1960)
                           hq  hm Ê  2 pq  1   6 pq  1     10 qq  ˆ
                        y =  -   Ásin   +   sin   +     sin    ˜        (4.13)
                              b  2 p  Ë  b  54  b   1250    b  ¯
                           1125
                       m =
                           1192
                           h  È  Ê  2 pq  1    6 pq  1    10 pq  ˆ˘
                               m
                       y ¢ =  Í 1 - Ácos  +  cos  +    cos    ˜ ˙
                              b  Î  Ë  b  18    b   250    b  ¯ ˚
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