Page 254 - Cam Design Handbook
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THB8  9/19/03  7:25 PM  Page 242

          242                      CAM DESIGN HANDBOOK

          Combining Eqs. (8.23) and (8.24) yields
                                      y
                                     Ê ˆ  2  y  d
                                sinq     -=   +   - cos .               (8.25)
                                          1
                                                     q
                                     Ë ¯     a  a
                                      r
          Squaring both sides of Eq. (8.25) and rearranging, we get
                                           2
                             Ê ˆ r  2  Ê ˆ  2  Ê ˆ Ê d  ˆ  2  2r  2  Ê d  ˆ
                                         r
                                    r
                     2
                   sin q -  sin q  =   +       - cosq  +     -  cosq  .  (8.26)
                           2
                             Ë ¯ y  Ë ¯  Ë ¯ Ë  a   ¯   ay  Ë  a  ¯
                                         y
                                    a
          Substituting for (1/y) from Eq. (8.21) into the above equation gives a quadratic equation
          in n
                 2
              Ê ˆ Ï Ê  d  - cosq ˆ  2  + sin q ¸  n - ) +1  2  r 2  2  Ê  d  - cosq ˆ ( n - ) +1  Ê ˆ  2  - sin q  = 0.
               r
                                                             r
                                  ˝ (
                                2
                                                                    2
              Ë  d ¯  Ì Ó Ë  a  ¯  ˛       ad Ë  a   ¯      Ë  a ¯
                                                                        (8.27)
          Several observations can be made about the above equation.
             1. Since Eq. (8.27) remains the same if we replace q with (2p - q), the two solutions
          of n for a given value of q correspond to the angular velocity ratios of the cam and the
          roller crank during the initial and reverse traversal of the roller on the cam. That is,
                                          Ê  df  ˆ
                                       n
                                n     ==
                                 solution1  Ë  dq  ¯  at 0
                                           Ê  df* ˆ
                                n solution2  = *  ˜   .                 (8.28)
                                       n = Á
                                           Ë  dq* ¯
                                                   2
                                                at 0* =( p 0
                                                    - )
             2. When q = 0 or p, Eq. (8.27) becomes independent of r
                                2                        2
                                        d d
                                                       d
                               ˆ
                          Ê  d  m 1 ( n 1) +  2 Ê  m 1 ( n 1)+  Ê ˆ  =  0.
                                               ˆ
                                     2
                                  -
                                                  -
                          Ë  a  ¯       a  Ë  a  ¯    Ë ¯               (8.29)
                                                       a
             This can be seen in Fig. 8.20 which shows the solution curves for n for different (r/d)
          ratios. It can also be observed in this figure that the region bounded by the two solution
          curves for one value of the (r/d) ratio contains similar curves of a larger ratio. As men-
          tioned earlier a larger value of (r/d) implies better transmission. Therefore, the region
          between two solution curves can be used to specify the angular velocity ratio n so that the
          transmission index (r/d) is larger than a minimum specified value. This is a useful feature
          in designing the mechanism.
             3. Figure 8.21 shows the solutions curves for n for a fixed ratio of (r/d) and varying
          ratios of (d/a). It can be seen that n = 0 occurs at the same two points. This is also evident
          from Eq. (8.27) if we substitute n = 0 and solve for q
                                   q
                               0
                            n =fi= sin   -1 ( r d) or  p  - sin  -1 ( r d)  (8.30)
          which is clearly independent of the ratio (d/a). This feature of the design (see Eq. [8.27])
          has  an  important  significance  if  a  long  dwell  or  reversal  of  motion  of  the  cam  is
          desired. That is, if we specify a lower bound on the transmission index (r/d), then the
          permissible region for n has zero or a negative value over only a limited range of q. For
          example,  the  maximum  possible  single  dwell  in  the  initial  traversal  of  the  roller
                            -1
          on the cam is (p - 2sin (r/d)). It should be noted that this is a minimum value of r here,
          not  r generically.  Thus,  the  ratio  is  useful  not  only  to  achieve  a  prescribed  minimum
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