Page 285 - Pipelines and Risers
P. 285

258                                                             Chapter 15


           15.2  Fracture of Pipes with Longitudinal Cracks
          The following assumptions are made for the analysis:


           0  Elastic-Plastic Fracture Mechanics is applied.
             The dent is assumed to be continuous and to have a constant length.
           0  The stress-concentrator is considered to be a notch located at the deepest point of the dent
             (infinite length, constant depth). The notch is longitudinal of length, k2c, and depth, a.

           15.2.1  Failure Pressure of Pipes with Longitudinal Cracks
          Longitudinal surface cracks can occur as isolated cracks or in colonies of  numerous closely
           spaced and parallel  cracks. A  procedure based on Maxey et al.  (1972)  for calculating the
          failure stress of longitudinal flaws is as follows:


          Folias factor MT is determined from Kiefner and Vieth (1989):
               MT  = 41 +0.6275x2-0.003375~~ for x 5 7.07                    (15.1)
               MT  = 0.032 x2 + 3.3      for x > 7.07                        (15.2)


           where:
               x=  U@t)'"
               L=  total length of the crack (G2c)
               D=  pipe nominal outside diameter
               t =  pipe wall-thickness.


           The failure pressure of pipes with longitudinal flaws is calculated as:
                   4t bfl,
               P, = -coi'(exp(-   B))                                        (15.3)
                   TCDMs

           where,  oflow is the  material  flow  stress and  auxiliary parameters MS and B  are given  as
           follows:

                                                                             (15.4)


                                                                             (15.5)


           where:
               a=   crackdcpth
               KmFmaterial toughness, estimated from Charpy impact energy tests, as shown later.
   280   281   282   283   284   285   286   287   288   289   290