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Realization of tin freezing point using a loop heat pipe-based hydraulic temperature control technique
14
Citations
12
References
2015
Year
EngineeringMechanical EngineeringExperimental ThermodynamicsHeat PipeRefrigerationFreeze-thaw CyclingChemical EngineeringSn FpThermodynamicsFreezing PlateausThermoanalytical MethodMaterials ScienceInside NucleationHeat TransferHigh Temperature MaterialsCryogenicsThermal ManagementThermal EngineeringThermophysical Property
In this work, the freezing point of tin (Sn FP) was realized by inside nucleation where the supercooling of tin and the reheating of the sample after the nucleation were achieved without extracting the cell from an isothermal apparatus. To this end, a novel hydraulic temperature control technique, which was based on the thermo-hydraulic characteristics of a pressure-controlled loop heat pipe (LHP), was employed to provide a slow cooling of the sample for deep supercooling and fast reheating after nucleation to minimize the amount of initial freeze of the sample. The required temperature controls were achieved by the active pressure control of a control gas inside the compensation chamber of the pressure-controlled LHP, and slow cooling at −0.05 K min−1 for the deep supercooling of tin and fast heating at 2 K min−1 for reheating the sample after nucleation was attained. Based on this hydraulic temperature control technique, the nucleation of tin was realized at supercooling of around 19 K, and a satisfactorily fast reheating of the sample to the plateau-producing temperature (i.e. 0.5 K below the Sn FP) was achieved without any temperature overshoots of the isothermal region. The inside-nucleated Sn FP showed many desirable features compared to the Sn FP realized by the conventional outside nucleation method. The longer freezing plateaus and the better immersion characteristics of the Sn FP were obtained by inside nucleation, and the measured freezing temperature of the inside-nucleated Sn FP was as much as 0.37 mK higher than the outside-nucleated Sn FP with an expanded uncertainty of 0.19 mK. Details on the experiment are provided and explanations for the observed differences are discussed.
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