Page 198 - Marine Structural Design
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174                                                      Part II Ultimate Strength


                                      0.05
                                      0.04              v; Reddy - steel '*)
                                                        m;  Reddy - alminium IC)
                                      0.03
                                    'cr
                                      0.02



                                      0.01
                                     0.008
                                     0.006
                                     0.005
                                     0.004

                                     0.003

                                     0.002



                                     0.001        &    I   I  l  l  I  1
                                                 20   30  40  50  60   80  100
                                                              Wt
                             Figure 9.15  Critical Buckling Strain



                       E,  = 0.4tfR                  for   /E,  2 2.5
                  Figure 9.15 shows the experimental critical buckling strains collected and arranged by Reddy
                  (1979). The critical buckling strain evaluated by Eq. (9.36) fall between two lines, 0.115  t/R
                  and 0.4 tlR, depending on the magnitude of E* f E, .


                  Post-Local Buckling Analysis
                  As described in Chapter 9.2,  local buckling takes place in  a cosine mode or a dent mode.
                  Accordingly, two kinds of analytical models are proposed, the  COS model and the DENT
                  model.
                  1. COS Model
                  Within  the  region  where  the  strain  in  the  axial  direction  exceeds  E,  , local  buckling
                  deformation is  assumed to  take place.  Its mode  in  the  axial  direction is approximated as
                  follows (See Figure 9.16 (a)):
                       Wb = (6/2XI-  cos(2m/s)j                                       (9.37)

                  where s represents the buckling wave length in the axial direction. Here, s is taken as 0.7 times
                  the wavelength of elastic buckling evaluated by the classical theory of elastic stability. That is
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