Page 84 - Mechanical Engineer's Data Handbook
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APPLIED MECHANICS                                                                  13

            2.4.4   Cams

            A cam is a mechanism which involves sliding contact
            and which converts one type of  motion into another,
            e.g.  rotary  to reciprocating.  Most  cams  are of  the
            radial type, but axial rotary cams are also used. Cams
            may have linear motion.  The motion is transmitted
            through  a  ‘follower’  and  four  types  are shown  for
            radial cams.













                                                        Circular arc cam with pat follower
                                                        On flank:
                                                        Lift y = (R -rl)(  1 -cos  e)
                                                        Velocity o=o(R-r,)  sin0
                                                        Acceleration a=w2(R-rl)  cos0
                                                        On nose:
                                                        Lift y = (r2 -  + d cos(a - e)
                                                                  r
                                                        Velocity  u = od sin@ - 0)
                                                        Acceleration a = - w2d cos(a - 0)
                                                        Maximum lift y,,=d-r,   +r,



            Tangent cam with roller follower

            On the flank:
            Lift y-  (rl + rJ(sec0-  1)
            where: 0=angle  of  rotation.
            Velocity v=w(rl +ro) sec0 tan0
                     d0
            where: w=-   the angular velocity.
                     dt
                                 (1 + 2 tanZ e)
            Acceleration a = w2(rl + r,)   cos e
            On the  nose: the  system  is  equivalent  to  a  con-
            rodlcrank mechanism with crank radius d and conrod
            length (ro+r2) (see Section 2.4.1).
            Maximum lift y,,,   = d - rl + r2
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