Page 71 - Thermal Hydraulics Aspects of Liquid Metal Cooled Nuclear Reactors
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46                    Thermal Hydraulics Aspects of Liquid Metal Cooled Nuclear Reactors


          Table 3.1 Physical properties of liquid metals and water at relevant temperatures

          Property      LBE       Pb         Na        H 2 O        Units
          Normal melting  125     327.5      97.8      0.0          °C
          point, °C
          Normal boiling  1654    1748       882       100          °C
          point, °C
          Properties at  400      400        400       25           °C
          1bar (temp.)
          Vapor pressure  3.44 10  5  3.04 10  5  5.20 10  5  3.17 10 3  Pa
          Density (ρ)   10,195    10,580     855.8     997.1        kgm  3
          Dynamic       1.514     2.227      0.277     0.890        mPas
          viscosity (μ)
                                                                       2  1
          Kinematic     0.15      0.21       0.32      0.89         mm s
          viscosity (ν)
          Heat capacity  142.9    146.7      1282.4    4182         Jkg  1  K  1
          (c p )
          Thermal       13.12     16.60      72.36     0.607        Wm  1  K  1
          conductivity (λ)
                                                                       2  1
          Thermal       9.01      10.70      65.93     0.1455       mm s
          diffusivity (a)
          Prandtl number  0.0165  0.0197     0.0049    6.137        –
          (Pr¼ν/a)
          Thermal       1.26 10  4  1.21 10  4  2.75 10  4  2.57 10  4  K  1
          expansion (β)
          Surface       394.6     449.8      166.0     72.0         mNm  1
          tension (σ)
          Source of data  OECD    OECD       Sobolev   Wagner and
                        (2015)    (2015)     (2010)    Kretzschmar
                                                       (2013)




         insulation to avoid freezing in all operational scenarios. Boiling, on the other hand, can
         usually be neglected. The high density of Pb and LBE impacts not only the weight of
         the facility but also the inertial forces at a given fluid velocity. This aspect must be
         taken into account for the analysis of, among others, local pressure losses and
         fluid-hammer effects. Due to the large thermal conductivity (λ) and diffusivity (a),
         larger heat flux densities are required in order to obtain temperature differences that
         can be accurately measured, resulting, for example, in more compact test sections.
            Further considerations are imposed by the liquid-metal chemistry, which is a broad
         research topic on its own, and it exceeds the scope of this chapter. An inert atmosphere
         is used for avoiding oxidation in contact with air or water, potentially representing a
         safety concern (e.g., sodium fires). The degradation of solid materials becomes more
         significant with increasing temperature, and technical solutions based on controlling
         the amount of dissolved impurities (mainly oxygen) are developed for achieving sat-
         isfactory compatibility with common materials, for example, stainless steel.
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