Page 181 - Thermal Hydraulics Aspects of Liquid Metal Cooled Nuclear Reactors
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Measurement techniques for liquid metal based nuclear coolants    153


                              Stopper
                       Tundish  rod
                       level

                                    Tundish




             z (mm)
                               Meniscus level
           335       1               8
                     2               9
           300
                     3              10
                     4              11
           250    X  5              12   X
                     6              13
           200
                     7              14
                     S               S
           150
           100
            50
             0
                                            –0.5 –0.4 –0.3 –0.2 –0.1 0.0  0.1  0.2 0.3 0.4 0.5
                        0    70  140 x (mm)
                                                            v (m/s)
           Fig. 3.5.6 Schematic sketch of the mold (A) of the mini-LIMMCAST facility equipped with 1
           excitation coil and 14 magnetic field sensors and a reconstruction of the velocity field in the
           mold for one instant in time (B).

           perturbation of one or more externally applied magnetic fields. From these measure-
           ments, the flow structure is reconstructed solving a linear inverse problem with an
           appropriate regularization technique. Besides the appropriate mathematical modeling
           of the inverse problem, the challenge of this technique is the reliable measurement of
           the tiny flow-induced magnetic field that is about three to five orders of magnitude
           smaller than the applied magnetic field. Therefore, a very stable current source for
           generating the excitation magnetic field and magnetic field sensors with a high
           dynamic range and a very linear response are needed. Using fluxgate probes and a
           static excitation magnetic field, it could be shown that the flow in the mold of a con-
           tinuous caster could be reconstructed with good agreement with accompanying UDV
           measurements (Wondrak et al., 2010, 2011). Fig. 3.5.6 shows a schematic sketch and
           the reconstructed velocity field in the mold of a model of a continuous caster. Success-
           ful measurements of the time-dependent behavior of the flow in a modified Rayleigh-
           B  enard setup showed the applicability of CIFT for very low velocities of about
           20mm/s (Wondrak et al., 2018). By using an AC excitation magnetic field with rather
           low frequency in the order of 1Hz, the flow-induced magnetic field can be separated
           from environmental noise suppressing undesired signals, for example, originating
           from moving ferromagnetic materials or from switching of electric currents in the
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