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          274                      CAM DESIGN HANDBOOK

          tion  of  protective  surface  films  to  reduce  wear  and  surface  damage. The  effectiveness
          of the films is established by their physical properties, which include shear strength, thick-
          ness, surface adhesion, film cohesion, melting point, and solubility. Operating variables
          that  affect  the  lubricant  include  load,  speed,  temperature,  and  environmental  atmos-
          phere. Additions in the lubricant include antiwear and antifoam agents, antioxidants, and
          viscosity improvers.
          9.5.2 Elastohydrodynamic Film (EHD)

          This section applies to roller followers only. Sliding followers are assumed to function in
          the boundary and mixed lubrication regimes. The elastohydrodynamic film is experienced
          by cast iron (with its free graphite and porosity) which operates with limited lubrication
          and gives good sliding and wear properties. Also, this section is written based on theories
          and tests from both rolling-element bearings and gearing (Zaretsky, 1997). Specific design
          data is not available for cam-follower elements. However, the information contained here
          is of a fundamental nature (rolling fatigue) so it can be applied to cams and followers since
          all these systems show similar surface fatigue wear. In application, some modifications
          and refinements may be necessary to account for the skidding action of the follower roller
          at high speeds and for larger cams. The information is presented as a potential design basis
          for the cam designer in selecting the best material and lubricant available and to optimize
          the performance of the machine. The important point is that the film that separates rolling-
          contact surfaces is elastohydrodynamic (EHD) film.
             Grubin (1949) solved the EHD problem by assuming that the elastic displacements of
          contacting  lubricating  surfaces,  heavily  loaded,  would  be  similar  to  the  dry  hertzian
          contact, Fig. 9.11.
             The dimensionless minimum film thickness is written as a function of the other three
          parameters
                                         f U W G)
                                      H = ( ,  ¢,
          which develops to
                                     h             -0091.
                                 H =   =195 G  073 ( W¢)                (9.16)
                                              .
                                         .
                                     R x
          in which G is the material parameter, U is speed parameter, and W¢ is the load parameter.
          The variables are related in Eq. (9.16) by four dimensionless groupings.
                            h
             Film thickness H =  ,  dimensionless
                            R
                             x
                              w
             Load parameter W ¢ =  ,  dimensionless
                               ¢ ER
                                x
             Speed parameter U =  u  E R ¢  ,  dimensionless
                              h 0  x
             Materials parameter G = a¢E¢, dimensionless
          where
                  h = EHD film thickness, in
                 R x = equivalent radius in the rolling direction, in
                 W¢= EHD load parameter, w/E¢R x
                 w = load per unit cylinder length, lb/in
                 E¢= effective Young’s modulus, lb/in 2
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