Page 219 - Pipelines and Risers
P. 219

192                                                               Chapter 12


          The true tension is an integration of  stress over the cross-section of  the steel wall. In deep
          water, Tp usually are greater than Ta. The result of  this is that Te becomes negative and the
          pipe section, as a beam, will be in compression instead of tension. The force T, is a function
          of the water depth so Te will always be positive at the sea surface and be positive or negative
          at the seabed depending on the relationship between T, and Tp.

           12.4.5 Curvature in Overbend
          The part of the pipeline that is supported by the layramp that are made up of the rollers placed
          on  the  stinger and  the  vessel  will  have  the  same curvature as  the  layramp.  A  target  for
          installation analysis is to find the best layramp configuration for the pipeline that is going to
          be installed.


          The layramp consists of  the lay-vessel and  the stinger. The function of  the layramp is to
          provide a curved support with an overall radius of  curvature. The result of  this is a bending
          moment in the pipeline and strain. This curve is created by placing out a number of rollers at
          the  barge  and  at  the  stinger. The  location  of  these  rollers  depends  on which  radius  of
          curvature that is needed to control the overbend-strain in the pipeline within acceptable level.


          The configuration and curvature of the pipe section are displacement controlled at the stinger.
          This means that the pipeline displacement is governed by the stinger and roller properties.


          The stinger and the vessel do not create a support with a constant curvature. This means that
          the bending moment is not constant along the pipeline on the stinger. The rollers/supports
          don’t create a continuos support for the pipeline. The result of  this is peaks in the moment
           level at every roller NOU (1974) and Igland (1997). The moment distribution over the stinger
           will therefore in principle be like illustrated in Figurel2.10.
                                         Moment distribution

                 Pipeline














           Figure 12.10 Moment distribution over stinger.

           It is therefore very important to represent the stinger geometry as accurate as possible in the
           finite element model.
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