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66                    Thermal Hydraulics Aspects of Liquid Metal Cooled Nuclear Reactors

         3.1.3.1 Mean flow and turbulence characteristics

         One of the first experimental studies on the mean flow in a rod bundle has been per-
         formed by Eifler and Nijsing (1967). They measured axial pressure drops along the
         bundle and local mean velocity at different wall distances with the help of a movable,
         very small (0.5 mm) Pitot tube (see Fig. 3.1.6).
            Pitot tubes were used by Seale (1979) as well, but measurements were performed in
         air instead of water. Seale combined the Pitot tube with a temperature sensor so that
         mixing of thermal energy could be analyzed as well. Obviously, putting a probe (such
         as a Pitot tube) inside the flow disturbs the flow itself and, therefore, influences the
         outcome. For this reason, Rowe (1973) applied, by then, the very new technique called
         laser Doppler velocimetry (LDV) or LDA. Much later, this technique has successfully
         been applied in rod bundles by, for example, McIlroy et al. (2008) and Mahmood et al.
         (2011). Besides LDA, McIlroy et al. used another optical technique, called PIV.
         Results can be found in the same reference (i.e., McIlroy et al., 2008). The major draw-
         back of optical techniques, such as LDV/LDA and PIV, is that the internals of the rod
         bundle need to be optically accessible and predictable. Light cannot pass through com-
         ponents like metal rods and is refracted when crossing two transparent materials of
         different refractive index (e.g., water and Perspex). Both the laser-based optical tech-
         niques and the solution to obtain proper optical access, called RIM, have been
         explained in Sections 1.2.4.1, 3.1.2.4.2, and 3.1.2.4.4, respectively.
            Turbulence, obviously, is a very important phenomenon in rod bundles, as heat
         transfer from the surface of the fuel to the bulk of the coolant flow is strongly



























         Fig. 3.1.6 Test channel as used by Eifler and Nijsing in 1967 to measure local mean
         velocities.
         (Adopted from Eifler, W., Nijsing, R., 1967. Experimental investigation of velocity
         distribution and flow resistance in a triangular array of parallel rods. Nucl. Eng. Des. 5(1),
         22–42.)
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