Page 175 - Marine Structural Design
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Chapter 8 Buckling/CoNapse of  Columns and Beam-columns                151


                                   e        e
                       N=bea, =bh-a,  =Np-                                            (8.65)
                                   h        h
                  Combination of Eqs. (8.64) and (8.65) gives

                                                                                      (8.66)


                  The above equation is the interaction formula for a rectangular cross-section under combined
                  axial load and bending.
                  Tubular Members
                  For tubular members, a fully plastic yielding condition for the cross-section may be obtained
                  as:
                       -  aP
                       M
                            cos(-.-)
                           =
                                                                                      (8.67)
                       MP
                  where,
                       Pp  =  crYA
                       M,  =  2lrRta,

                  where R is radius of the cross-section.

                  8.4  Examples

                  8.4.1  Example 8.1: Elastic Buckling of Columns with Alternative Boundary Conditions
                  Problem:
                  Derive elastic buckling strength equation based on the basic differential equation for initially
                  straight columns:
                       d4w     d2w
                       -+k2--      -0                                                 (8.68)
                       dr4     dx2
                  Solution:
                  The general solution of Eq. (8.68) is:
                       w = Asin kx i Bcoskx -I- Cx + D                                (8.69)
                  (1) Columns with Hinged Ends
                  The deflection and bending moments are zero at both ends:
                          d2w
                       w=-=O      at  x=O  and  x=l                                   (8.70)
                          dx2
                  Applying the boundary conditions to the general solution, we may get:

                       B=C=D=O  sinkl=O                                               (8.71)
                  Hence,
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