Abstract

In future fusion reactors tritium and deuterium will be used as a primary fuel. Currently, the most important research and development project about nuclear fusion energy is the ITER (International Thermonuclear Experimental Reactor). To produce the fusion reaction, tritium will be generated inside the core using a breeding blanket. One of the suggested blankets is based on the use of molten lithium – lead eutectic alloy (Pb-15.7Li) [1]. This blanket will be flowing around the reactor core and while the fusion reaction occurs, energy is released and collected with an external heat exchanger system.Due to its short half-life (12.3 years), there are not natural tritium sources. Therefore, it must be obtained in situ and continuously in the breeding blanket. This hydrogen isotope can be produced by bombarding lithium with fast neutrons, which escape from the generated and confined plasma in the toroid-shaped vacuum chamber of a tokamak, to yield tritium and helium (6Li + n → 4He + 3H + 4.8MeV) [2]. Hence, dynamic tritium concentration measurement is of major interest for nuclear fusion reaction engineering and for an experimental proof of tritium self-sufficiency in liquid metal breeding systems. Consequently, it is necessary a measuring system that allows to determine tritium concentration in high temperature conditions.Electrochemical sensors based on solid-state proton conductor ceramics can be used for that purpose. These materials have attracted significant interest because of their chemical and physical durability, especially at elevated temperatures. These electrolytes are perovskite type materials with electrical carriers, positive holes, excess electrons, oxide ion vacancies and interstitial protons, which interact with oxide ions. Under this approach, new methods of synthesis are being studied in order to obtain ceramic materials of higher quality and purity able to offer better measurement signals.In the present work, the proton conducting perovskite Sr(Ce0,9-Zr0,1)0,95Yb0,05O3-α was synthesized by two different methods. On one side, a conventional sol-gel method was employed [3]. On the other hand, the ceramic particles were synthesized by flame spray pyrolysis. Structural phases were determined by X-Ray Diffraction. The powder obtained with both methods showed a single phase of the perovskite-type and good agreement with bibliography data.Finally, the obtained ceramic materials were properly sintered and shaped in order to construct electrochemical hydrogen sensors. Amperometric measurements were performed at 500 ºC using different hydrogen partial pressures and the response of the two sensors was compared.

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