Page 216 - Marine Structural Design
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192                                                      Part II Ultimate Strength

                 represent  the  results  obtained  from  the  finite element  method  without  considering local
                 buckling.
                 Until local buckling takes place, both results obtained from the present method and the finite
                 element method, show good correlation's including the ultimate strength. The comparison of
                 these results using the FEM to the results of other experiments shows little differences among
                 them, which may be attributed to the reasons described in 9.4.1. However, judging from the
                 interaction relationships shown in Figure 9.29, these  differences may  be  attributed to  the
                 material properties of the actual material and assumed material used for the analysis. The yield
                 stress used  in the analysis is determined, based on the results of the tensile test, and may be
                 very accurate as long as the stress is in tension. It is not completely clear, but there may be
                 some differences in the material properties in a tensile and a compressive range.




                                   :
                              _-__-- ANAL
                              -:     ISM
                              --- FEM
                                   :









                          -1.0   -0.8   -0.6   -0.4   -0.2   0   0.2   0.4   0.6   0.8   1.0
                                                                       Wp

                            Figure 9.27  Axial Force Bending Moment Relationships
                 Post-local buckling behavior is simulated quite well although the calculated starting points of
                 local buckling are a little different from the measured ones. The difference in the onset point
                 of local buckling may  be  due to  inaccuracies of the  critical buckling strain evaluated by
                 Eq.(9.31) and the estimated strain using Eq.(9.67). At present, the value to be employed as n
                 remains unknown. Although larger values may give good results as indicated in Figures 9.28
                 and 9.29.
                 The  curves  changing  the  value  of  n  may  be  regarded  as the  results  of  the  numerical
                 experiment, changing the onset point of local buckling. A greater reduction is observed in the
                 load canying capacity (axial load) as the critical load for buckling increases.
                 The same analysis is performed on small-scale test specimens. Relatively good correlation's
                 are observed between the calculated and experimental results for the ultimate strength in all
                 specimens. However, the calculated post-ultimate strength behavior is slightly different from
                 the observed behavior.  This may be  attributed to  a difference in the  assumed stress-strain
                 relationship used during the analysis and  the actual one. An  elastic-perfectly plastic stress-
                 strain relationship is assumed in the analysis. Contrary to this, the actual material showed
                 relatively  high  strain  hardening.  In  order  to  analyze  such  cases,  the  influence of  strain
                 hardening must be taken into account. The strain hardening effect may be easily incorporated
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