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TERMINAL OPERATIONS



                    16.8      Generation of Pressure Surges in Pipelines
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                              16.8.1    Introduction

                                        A pressure surge is generated in a pipeline system when there is an
               งานห้องสมุด ศูนย์ฝกพาณิชย์นาวี
                                        abrupt change in the rate of flow of liquid in the line. In tanker loading
                                        operations, it is most likely to occur as a result of one of the following:
                                          Closure of an automatic shutdown valve.

                                          Slamming shut of a shore non-return valve.
                                          Slamming shut of a butterfly type valve.
                                          Rapid closure of a power operated valve.

                                        If the pressure surge in the pipeline results in pressure stresses or
                                        displacement stresses in excess of the strength of the piping or its
                                        components, there may be a rupture, leading to an extensive spill of oil.



                              16.8.2    Generation of a Pressure Surge
                                        When a pump is used to convey liquid from a feed tank down a pipeline
                                        and through a valve into a receiving tank, the pressure at any point in the
                                        system while the liquid is flowing has three components:
                                                                          ึ
                                          Pressure on the surface of the liquid in the feed tank. In a tank with its
                                           ullage space open to atmosphere, this pressure is that of the
                                           atmosphere.

                                          Hydrostatic pressure at the point in the system in question.
                                          Pressure generated by the pump. This is highest at the pump outlet,
                                           decreasing commensurately with friction along the line downstream of
                                           the pump and through the valve to the receiving tank.

                                        Of these three components, the first two can be considered constant
                                        during pressure surge and need not be considered in the following
                                        description, although they are always present and have a contributory
                                        effect on the total pressure.

                                        Rapid closure of the valve superimposes a transient pressure upon all
                                        three components, owing to the sudden conversion of the kinetic energy
                                        of the moving liquid into strain energy, by compression of the fluid and
                                        expansion of the pipe wall. To illustrate the sequence of events, the
                                        simplest hypothetical case will be considered, i.e. when the valve closure
                                        is instantaneous, there is no expansion of the pipe wall, and dissipation
                                        due to friction between the fluid and the pipe wall is ignored. This case
                                        gives rise to the highest pressures in the system.

                                        When the valve closes, the liquid immediately upstream of the valve is
                                        brought to rest instantaneously.

                                        This causes its pressure to rise by an amount P. In any consistent set of
                                        units:
                                                P = wav
                                        where: w is the mass density of the liquid
                                                a is the velocity of sound in the liquid
                                                v is the change in linear velocity of the liquid, i.e. from its linear
                                                flow rate before closure.





                                                   © ICS/OCIMF/IAPH 2006                                       257
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