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THB4  8/15/03  1:01 PM  Page 93

                            POLYNOMIAL AND FOURIER SERIES CAM CURVES        93

                       TABLE 4.1  Zero Coefficient Terms

                       Powers in         Zero derivatives  Powers in
                       general polynomials  (at 0 = 0)  remaining terms
                       0 and 1             None            1
                       0 to 3              y               2, 3
                       0 to 5              y¢, y≤          3, 4, 5
                       0 to 7              y¢, y≤, y       4, 5, 6, 7




            These eight conditions establish the general polynomial
                                 q
                         y =  C +  C +  C q  2  + C q  3  +  C q  4  +  C q  5  +  C q  6  +  C q .
                                                                7
                                0  1  2   3    4    5    6     7
            In dealing with high-degree polynomials, simplifications can be made if we realize that
                      dy
                       n
            when q = 0,   = 0 . Subsequently, the coefficient for that derivative is C n = 0. This is
                      dq  n
            summarized in Table 4.1 for polynomials thus far derived for the DRD event.
               For the 4-5-6-7 polynomial, C 0 = C 1 = C 2 = C 3 = 0. The remaining conditions at q = 1
            give the following equations:
                                          C +  C +  C + C = 1
                                             4  5  6  7
                                      4C +  5C +  6C +  7C =  0
                                        4    5   6    7
                                            +
                                  12C + 2030C +    42C =  0
                                          C
                                      4    5    6     7
                                 24C +  60120C +  210C =  0.
                                          +
                                        C
                                     4   5     6      7
            Solving these simultaneously for the 4-5-6-7 polynomial yields
                                               q
                                                 -
                                                6
                                   y = 35q  4  -84q  5  + 7020q  7
                                     q
                                       -
                                      3
                                   y ¢ =140420q  4  + 420q  5  -140q  6
                                       -
                                     q
                                      2
                                  y ¢¢ = 4201680q  3  + 2100q  4  -840q  5
                                                           4
                                    y ¢¢¢ = 840q  - 5040q  2  + 8400q  3  - 4200q .  (4.5)
            Figure 4.3 shows a plot of these curves.
               If we compare this acceleration curve with the lower order 3-4-5 polynomial, we see
            larger maximum acceleration and larger maximum jerk values. This indicates a possible
            inferiority to the 3-4-5 polynomial. A zero value of jerk is not required since manufactur-
            ing limits generally cannot meet this control. Next, let’s compare the physical significance
            of the 4-5-6-7 polynomial. Table 4.2 shows the dynamic comparison with the 3-4-5 poly-
            nomial, basic simple harmonic, and cycloidal curves.
               The physical meaning of this controlled acceleration is best depicted by large-scale
            plotting of the curves. Figure 4.4 compares these curves with an expanded view of the end
            points. The data is based on 2 percent of follower rise and 14 percent of cam rotation.
            Further control of fourth and higher derivatives raises the maximum acceleration and also
            the time consumed for the initial and final displacement of the cam, and manufacturing
            limits are often demanded.
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