Page 214 - Marine Structural Design
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190                                                     Pari N Ultimate Strength


                                                     :
                                              - Experlent
                                        0.6  r  ------- : COS  -del












                                                                 c/ cy
                             Figure 9.25  Comparison of Calculated and Measured Results (S3)

                  9.4.2  Idealized Structural Unit Method Analysis
                  Members with Constraints against Rotation at Both Ends
                  An end rotation of a structural member in a structural system is constrained by other members.
                  This effect of constraint may be equivalent to placing springs, which resist rotation at both
                  ends of a member when one member is isolated from the system. For such a member with
                  springs at both  ends,  a  series of  analyses are performed  by changing the  spring constant
                  between 0 and 00.  The wall thickness and outer diameter are taken as 20 mm and 2,000 mm,
                  respectively. The initial deflection of magnitude MOO times the length is imposed to know the
                  characteristics of the proposed Idealized Structural Unit model. The yield stress of the material
                  is chosen as 30 kgf7mm2, and the magnitudes of springs at both ends are the same. Local
                  buckling is not considered in this analysis. The calculation results for r/m =loo are shown
                  in Figures 9.26  and 9.27.  Figure 9.26 represents the load vs. lateral deflection relationships,
                  and Figure 9.27 represents the change of internal forces at a mid-span point and end. In these
                  figures, the  solid  lines and chain lines represent the results obtained by  using the present
                  method  and  the  finite  element method, respectively.  On  the  other hand,  the  dashed  lines
                  represent the analytical solutions expressed as follows:
                  Perfectly elastic solution
                       w= 2M[l/(2cosW/2)-1]+a0  P,/(P,  -P)                           (9.97)
                  where,

                                                                                      (9.98)

                  and k represents the magnitude of springs placed at both ends, and PE is given in Eq. (9.6).
                  Rigid plastic solution
                       w = M, [co~(~P/~P,)]/P for &O                                  (9.99)

                       w = 2kt,[cos(n~/~~,)l/~ for kco                               (9.100)
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