Page 196 - Thermal Hydraulics Aspects of Liquid Metal Cooled Nuclear Reactors
P. 196

System thermal hydraulics for liquid metals                       167


           and then

                                 v     T _ v
                                  2      2
                 ∂v l             l, ref  l, ref        dv l, ref            2
                      ¼ F 1 TðÞ ¼             with _ v l, ref    ¼ b 1 +2b 2 T +3b 3 T
                 ∂p             w 2                      dT
                    T             sl, ref  c pl, ref
           Deriving again with respect to the temperature, the following correlation is obtained:


                _     dF 1 TðÞ  d  ∂v l
               F 1 TðÞ      ¼
                        dT    dT ∂p
                                      T
                        2v l, ref _ v l, ref w sl, ref  2 _ w sl, ref v 2 l, ref
                    ¼
                                  w 3
                                   sl, ref
                           2                       2
                         _ v  +2T _ v l, ref € v l, ref c pl, ref  T _ v  _ c
                          l, ref                   l, ref pl, ref
                                        2
                                       c
                                        pl, ref
           where:
                    2
                    d v l, ref                 dw sl, ref
              € v l, ref    2 ¼ 2b 2 +6b 3 T,  _ w sl, ref    ¼ c 1 +2c 2 T,  and  _ c pl, ref
                     dT                         dT
                               2
           dc pl, ref  ¼ d 1 +2d 2 T +3d 3 T .
            dT
              Finally, the partial derivative of the specific volume with respect to the temperature is

                 ∂v l         _
                      ¼ _ v l, ref + F 1 TðÞ p p ref
                 ∂T
                     p
           The thermal expansion coefficient and the isothermal coefficient of compressibility
           can be then calculated according to their definitions:
                                                        _

                          1     ∂v l           _ v l, ref TðÞ + F 1 TðÞ p p ref
                                        ð
               β T, pð  Þ           ) β T, pÞ ¼
                l
                                        l
                        v l T, pð  Þ ∂T               v l T, pð  Þ
                                   p

                            1    ∂v l              F 1 TðÞ
                                          ð
               κ l T, pð  Þ           ) κ l T, pÞ ¼
                         v l T, pð  Þ ∂p          v l T, pð  Þ
                                     T
           Similar derivations can be used to obtain the specific enthalpy, the specific internal
           energy, and the specific entropy of the liquid phase as a function of both temperature
           and pressure.
           4.3.2 Vapor phase
           In principle, in STH codes, the properties of coolants in vapor phase are also needed.
           Apart from the sodium, the other liquid metals foreseen in the nuclear field as possible
           coolants (such as lead and lead-bismuth) have the boiling temperature so high that
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