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Nuclear Production of Hydrogen, Fourth Information Exchange ...

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HIGH-TEMPERATURE STEAM ELECTROLYSIS FOR HYDROGEN PRODUCTION: FROM MATERIAL DEVELOPMENT TO STACK OPERATION<br />

Nd 2 NiO 4+δ powder was prepared by nitrate-citrate route as described by Courty, et al. (1973).<br />

Stoichiometric amounts <strong>of</strong> neodymium and nickel oxides were dissolved in diluted nitric acid. After<br />

addition <strong>of</strong> a large excess <strong>of</strong> citric acid, the solution was dehydrated and heated until self-combustion<br />

<strong>of</strong> the precipitate to obtain submicronic precursor particles (Boehm, 2005). The final annealing was<br />

performed at 1 000°C for 12 hours to obtain a single crystalline phase. The particles were then ball milled<br />

to obtain an average grain size (d 0.5 ) <strong>of</strong> about 0.8 μm. A terpineol-based slurry was prepared from this<br />

powder and this was deposited on the electrolyte by screen printing and then sintered at 1 100°C for<br />

three hours in air (Lalanne, 2008).<br />

Nd 2 NiO 4+δ was manufactured at ICMCB and deposited by screen printing on half electrolyte<br />

supported cells made <strong>of</strong> Ni-CGO hydrogen electrode and TZ3Y electrolyte, 90 μm thick. The thickness<br />

<strong>of</strong> the final Nd 2 NiO 4+δ porous layer was about 30 μm (Figure 2).<br />

Figure 2: SEM micrograph <strong>of</strong> the Ni-CGO/TZ3Y/Nd 2 NiO 4+δ cell after study<br />

Nd 2 NiO 4+δ<br />

TZ3Y<br />

Ni-CGO<br />

Performance <strong>of</strong> the cells containing Nd 2 NiO 4+δ oxygen electrode was compared to reference cells<br />

made <strong>of</strong> the same electrolyte (TZ3Y, 90 μm thick) and a Ni-CGO hydrogen electrode but containing a<br />

classical LSM oxygen electrode.<br />

For these characterisations, the inlet gas composition to the hydrogen electrode was composed <strong>of</strong><br />

hydrogen (37%), water vapour (35%) and argon (28%), the total flow rate being 10.7 L.h –1 . The inlet gas<br />

to the anode side was air (7 L.h –1 ). Current collectors on both positive and negative electrodes were<br />

gold grids (1 024 meshes.cm –2 ) and platinum grids (3 600 meshes.cm –2 ), with the platinum grid being<br />

directly in contact with the electrodes. This assembly aims to have a good contact with electrodes.<br />

Measurements were performed at 750°C, 800°C and 850°C, from the lowest to the highest temperature.<br />

i--V curves were recorded under galvanostatic control from open circuit cell voltage (OCV) to the<br />

highest polarisation, then back to OCV.<br />

Results analysis<br />

Performances are evaluated using area specific resistance (ASR) calculated at 1.3 V (slope <strong>of</strong> i-V curve<br />

between 1.25 and 1.35 V), and using the quantity <strong>of</strong> hydrogen produced at 1.3 V (nominal voltage) and<br />

at 1.5 V (maximum voltage) according to Faraday’s law. The steam utilisation rate is also calculated as<br />

the molar amount <strong>of</strong> hydrogen produced (according to Faraday’s law and assuming 100% current<br />

efficiency) divided by the molar amount <strong>of</strong> water in the inlet cathodic gas.<br />

The degradation rate is calculated from the voltage curve versus time and given as a percentage<br />

<strong>of</strong> voltage loss per time unit.<br />

122 NUCLEAR PRODUCTION OF HYDROGEN – © OECD/NEA 2010

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