Page 75 - Pipelines and Risers
P. 75

48                                                                 Chapter 3


           Here the two failure modes work against each other and thereby “strengthen” the pipe. For
            high internal overpressure, the collapse will always be initiated on the tensile side of the pipe
           due  to  stresses  at  the  outer  fibers  exceeding  the  material  limit  tensile  stress.  On  the
           compressive side of the pipe, the high internal pressure will tend to initiate an outward buckle,
            which will increase the pipe diameter locally and thereby increase the moment of inertia and
            the bending moment capacity to the pipe. The moment capacity will therefore be expected to
           be higher for internal overpressure compared with a corresponding external pressure.
            3.3.2  Combined External Pressure and Bending

           Bai  et  al.  (1993,  1994,  1995  and  1997)  conducted  a  systematic  study  on  local
            buckling/collapse of external pressurized pipes using the following approach:


              review experimental work
              validate finite element (ABAQUS) models by  comparing numerical results with  those
              from experimental investigation
              conduct extensive simulation of buckling behavior using validated finite element models
              develop parametric design equations accounting for major factors affecting pipe buckling
              and collapse
              estimate  model  uncertainties by  comparing the  developed  equations  with  the  design
              equations


           Details of the equations are given in the above listed papers, in particular Bai et al. (1997).

            The ultimate strength equations for pipes under combined external over-pressure and bending
                (e)a +(g                                                      (3.22)
            is proposed by Bai (1993) as the following function:
                               1
                              =


            In experimental tests, sets of W) and (P/Pc) at failure are recorded. The exponents a and B
            can be optimized by identifying which  values of  a and p will provide the most stable and
            consistent  probabilistic  description  of  the  model  uncertainty  in  terms  of  mean  value
            (preferably close to  l.O),  CoV (as low  as possible) and distribution type (preferably with  a
            distinct lower bound).

            Based  on finite element results,  Bai  et  al.  (1993) proposed  that  a = p=1.9. In  DNV’96
            pipeline rules, a round number 2.0 is adopted.

            In  order to develop simple criteria for bucklingkollapse of  pipelines under  simultaneously
            axial force, pressure and bending, formulation described in  Section 3.4 is used  (Hauch and
            Bai, 1999). See ABS(2000).
   70   71   72   73   74   75   76   77   78   79   80