Page 166 - Thermal Hydraulics Aspects of Liquid Metal Cooled Nuclear Reactors
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138                   Thermal Hydraulics Aspects of Liquid Metal Cooled Nuclear Reactors

         moves, the bellow maintains a seal and significantly reduces leakage probability com-
         pared with conventional valve designs with gland packing.
            However, the bellows used in these valves have to be relatively thin, such as a few
         tenths of a millimeter, to allow flexibility. Due to the volume change during LBE
         solidification, freezing liquid metal in the confined space of a valve body/bonnet
         should be avoided to prevent damage to the delicate bellow. If solidification is
         unavoidable for some reason, particular precautions should be taken not to operate
         the valve so that the bellow is not overstressed. Automated valves should be inter-
         locked not to actuate below a set point close to the melting point. This limit could
         be 150°C for LBE and 380°C for lead.


         3.4.9.2 Pressure surge
         Pressure surge, or fluid hammer, is a pressure transient caused by a sudden change in
         fluid velocity, that is, fluid momentum change. The phenomenon of pressure surge is
         not unique to liquid metals but applicable to many fluid network systems. Yet, as will
         be shown, the high density of LBE (and all other HLM) makes the phenomenon of
         fluid hammer an important consideration in the design and operation of HLM facil-
         ities. Fluid hammer can occur when a valve closes too quickly or a pump starts with an
         empty discharge line or stops suddenly during a pump trip. The result is the establish-
         ment of pressure waves that are potentially significantly higher than the normal oper-
         ating pressure, which can cause severe vibration, piping strain, and even pipe or
         component rupture.
            The maximum possible pressure rise (potential surge) associated with a fluid ham-
         mer event is simply determined from the well-known Joukowski equation, which
         assumes an instantaneous valve closure in frictionless pipes (Thorley, 2004). The
         Joukowski equation is given by Eq. (3.4.2):

             ΔP ¼ ρ c ΔV                                                (3.4.2)

         where
            ΔP¼surge pressure rise (Pa)
                            3
            ρ¼fluid density (kg/m )
            c¼pressure wave speed (m/s)
            ΔV¼change in fluid velocity (m/s)
         The assumption of instantaneous valve closure is conservative with respect to the
         surge pressure rise. For more accurate estimations, more analysis is required. The
         pressure wave velocity and hence the magnitude of the surge pressure wave also
         depend upon the piping restraint characteristics, the modulus of the pipe material,
         and the modulus of elasticity of the liquid. While the pressure wave speed (c) is depen-
         dent on the pipeline elasticity characteristics, the pressure rise is directly proportional
         to the fluid density. Considering the high density of LBE, an instantaneous valve clo-
         sure in an LBE facility would produce a potential surge pressure rise approximately
         10 times greater than a water facility with the same initial flow velocity and piping
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