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84 Reliability and Maintainability of In-Service Pipelines


              samples are generated. Monte Carlo method is the major simulation method
              for structural reliability analysis of pipelines.
              FORM techniques: In First-Order Reliability Methods (FORM) the limit state
              function (failure function) is linearized and the reliability is estimated using
              level II or III methods.
              SORM techniques: In Second-Order Reliability Methods (SORM) a quadratic
              approximation to the failure function is determined and the probability of fail-
              ure for the quadratic failure surface is estimated.
              Time-dependent reliability techniques: When a pipeline is subjected to a time-
              dependent degradation process, probabilistic time-dependent methods can be
              used. First passage probability theory has been introduced for time-dependent
              reliability analysis (Melchers 1999). Gamma process concept also has the
              potential of usage as a model for reliability analysis of pipelines subject to
              monotonic degradation processes (Mahmoodian and Alani 2014). These meth-
              ods are discussed and developed in Chapter 4, Time-Dependent Reliability
              Analysis, for reliability analysis of pipelines.

              For a detailed introduction to structural reliability theory references are made
           to the following textbooks: Melchers (1999), Thoft-Christensen and Baker (1982),
           and Ditlevsen and Madsen (1996).




              3.3 Generalization of a Basic Reliability Problem

           In a basic reliability problem only one load effect, S, can be resisted by one resis-
           tance, R. The load and the resistance are expressed by a known probability den-
           sity function, f S and f R , respectively.
              Considering the definition of safety, the pipeline will be marked as failed if its
           resistance, R, is less than the stress resultant, S, action on it. Therefore the proba-
           bility of failure can be stated as follows:
                              P f 5 PR 2 S # 0Š 5 PGðR; SÞ # 0Š           ð3:2Þ
                                    ½
                                                ½
           where GðR; SÞ is termed the limit state function, and the probability of failure is
           identical to the probability of limit state violation. In Fig. 3.1, the above equation
           is represented by the hatched failure domain D, so that the failure probability
           becomes (Melchers 1999):

                                              ð ð
                             P f 5 PðR 2 S # 0Þ 5  f RS ðr; sÞdrds        ð3:3Þ
                                               D
           where f RS ðr; sÞ is the joint (bivariate) density function.
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