Page 370 - Cam Design Handbook
P. 370

THB12  9/19/03  7:34 PM  Page 358

          358                      CAM DESIGN HANDBOOK

             Models with a relatively rigid camshaft are the most general. Models with an elastic
          camshaft are an occasional requirement. Models with an elastic camshaft are coupled to
          the  follower  resulting  in  nonlinear  second-order  differential  equations,  since  the  cam
          movement on the shaft is not a direct function of time.
             Multi-degree-of-freedom systems are shown, but note that they are shown to be com-
          plicated and difficult to apply, time-consuming, and thus costly. It has been found that the
          one-degree-of-freedom model is satisfactory as long as the excitations of the second and
          higher modes are much less than those near the first mode, which is usually true. The rep-
          resentation of a cam-follower mechanism by means of a single-degree-of-freedom model
          having a natural frequency equal to the fundamental natural frequency of the actual system
          is  satisfactory.  The  fundamental  natural  frequency  dominates  the  transient  follower
          responses, which are treated in Chap. 13. Most researchers involved with the dynamics of
          cam-follower systems use linear one-degree-of-freedom spring-mass models with either
          open or closed-track cams for constraint of the follower. The closed-track cam is pre-
          dominantly  utilized  for  production  machinery,  and  the  open-track  cam  (spring  force
          loaded) is specifically used for automotive valve gear systems. Nonlinear stiffness models
          have rarely been used, since the nonlinear component of the stiffness is usually relatively
          small. In addition, nonlinearities caused by passive parameters are not addressed in this
          book. These nonlinearities are damping of various kinds (e.g., Coulomb friction, quadratic
          damping, stiction, and combinations), backlash, and tolerances in mechanical components.
          The nonlinear models must be solved numerically with Runge-Kutta and Adams Bulirsch-
          Stoer algorithms. The Runge-Kutta Methods are the most popular; for other choices. Chen
          (1982), Chen and Polvanich (1975a,b), and Koster (1970) have employed computer sim-
          ulations using models of complex cam systems including multiple nonlinear component
          effects.
             The following are the commercially available computer programs:
             TK Solver, Universal Technical Services
               1220 Rock Street
               Rockford, Ill. 61101
               www.uts.com
             Mathcad, Mathsoft, Inc.
               101 Main Street
               Cambridge, Mass. 02142
               www.mathsoft.com
             MATLAB/SIMULINK, The Mathworks, Inc.
               2W Prime Parkway
               Natick, Mass. 01760
               www.mathworks.com



          12.2 SYSTEM VIBRATIONS

          This section looks at the practical and theoretical sources of vibration that may occur in
          the design and study of high-speed cam-follower mechanisms. This information is item-
          ized to enhance the knowledge of the theoretical simplified modeling that is used. Although
          simplified models are invaluable, the designer should not be “trapped” totally by conclu-
          sions that models reveal. One should always maintain freedom of thought in the process
          of designing high-speed machinery. All vibrations are not always what the model reveals
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