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FINITE ELEMENT MODELING
OF GOLF IMPACTS
April 3, 2009
Completed By: Doug Alguire
Supervisor: John McPhee
Construction
      Hypermesh was used to create golf ball model, then material properties
       and rigid plate model were defined with batch files in Ansys 11.0
      Ball material properties and impact conditions taken from work by Tanaka
       et al. [1]




                                                                          Component                         Radius (mm)                          Properties


                                                                              Core                               17.7                   Hyperelastic +Viscoelastic


                                                                            Mantle                               19.4                   Hyperelastic +Viscoelastic


                                                                             Cover                               21.4                           Hyperelastic




    [1] Tanaka, K., Sato, F., Oodaira, H., Teranishi, Y. and Ujihashi, S. (2006). Construction of the finite- element models of golf balls and simulations of their
        collisions, Proc. IMechE Vol. 220 Part L: Journal of Materials: Design and Applications, pp13-21.
Impact Simulations
   Normal and oblique impacts were simulated
       Oblique impacts achieved by adding z-component to initial
        ball velocity (as opposed to angling the plate)
Normal Impact Results
   Contact time decreases with increasing initial velocity (ranged from ~0.58
    to 0.64 ms, contact time for 44.4 m/s (99.3 mph) initial velocity is shown
    below)


                           Impact
Normal Impact Results (Cont’d)
   The FE model results showed close agreement with the
    experimental results of Tanaka et al. for all three impact
    velocities studied

                                 Experimental      New FE Model
              Initial Velocity
                               Rebound Velocity   Rebound Velocity
                   (m/s)
                                   (m/s) [1]           (m/s)

                  24.9              21.1                20.9
                  34.5              27.9                27.8
                  44.4              34.2                34.1
Oblique Impact Results
   Simulation results and post-processing were validated by the consistency of
    the post-impact angular velocity (note: angle of incidence=30°, initial
    velocity=45.0 m/s)
Oblique Impact Results (Cont’d)
   FE model results are adequate, but tend to overestimate backspin
       Discrepancies increase at higher loft angles but remain relatively constant for
        various impact velocities, suggesting that the friction model is the source of the
        problem
Summary
   Utilized Ansys to recreate the work done by
    Tanaka et al.
   Achieved a high level of agreement between FE
    model and experimental results
   Further work needed to investigate the friction
    model to improve oblique impact results

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FE Modelling Of Golf Impacts, by Doug Alguire

  • 1. FINITE ELEMENT MODELING OF GOLF IMPACTS April 3, 2009 Completed By: Doug Alguire Supervisor: John McPhee
  • 2. Construction  Hypermesh was used to create golf ball model, then material properties and rigid plate model were defined with batch files in Ansys 11.0  Ball material properties and impact conditions taken from work by Tanaka et al. [1] Component Radius (mm) Properties Core 17.7 Hyperelastic +Viscoelastic Mantle 19.4 Hyperelastic +Viscoelastic Cover 21.4 Hyperelastic [1] Tanaka, K., Sato, F., Oodaira, H., Teranishi, Y. and Ujihashi, S. (2006). Construction of the finite- element models of golf balls and simulations of their collisions, Proc. IMechE Vol. 220 Part L: Journal of Materials: Design and Applications, pp13-21.
  • 3. Impact Simulations  Normal and oblique impacts were simulated  Oblique impacts achieved by adding z-component to initial ball velocity (as opposed to angling the plate)
  • 4. Normal Impact Results  Contact time decreases with increasing initial velocity (ranged from ~0.58 to 0.64 ms, contact time for 44.4 m/s (99.3 mph) initial velocity is shown below) Impact
  • 5. Normal Impact Results (Cont’d)  The FE model results showed close agreement with the experimental results of Tanaka et al. for all three impact velocities studied Experimental New FE Model Initial Velocity Rebound Velocity Rebound Velocity (m/s) (m/s) [1] (m/s) 24.9 21.1 20.9 34.5 27.9 27.8 44.4 34.2 34.1
  • 6. Oblique Impact Results  Simulation results and post-processing were validated by the consistency of the post-impact angular velocity (note: angle of incidence=30°, initial velocity=45.0 m/s)
  • 7. Oblique Impact Results (Cont’d)  FE model results are adequate, but tend to overestimate backspin  Discrepancies increase at higher loft angles but remain relatively constant for various impact velocities, suggesting that the friction model is the source of the problem
  • 8. Summary  Utilized Ansys to recreate the work done by Tanaka et al.  Achieved a high level of agreement between FE model and experimental results  Further work needed to investigate the friction model to improve oblique impact results