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High Temperature Electrolysis Coupled to Nuclear Energy for Fuels Production and Load Following Bilge Yildiz, Mujid Kazimi, Charles Forsberg Massachusetts Institute of Technology Department of Nuclear Science and Engineering


  1. High Temperature Electrolysis Coupled to Nuclear Energy for Fuels Production and Load Following Bilge Yildiz, Mujid Kazimi, Charles Forsberg Massachusetts Institute of Technology Department of Nuclear Science and Engineering Tsinghua-Cambridge-MIT Low Carbon Energy University Alliance Video Conference January 13, 2010 1

  2. Electricity and hydrogen / syn-gas co-generation •CO 2 -free Nuclear Electrolysis and Energy •Efficient and cost- Fuel cell processes: competitive H 2 O (g) �� ½ O 2(g) + H 2(g) •Size/location to address the industry needs Co-electrolysis: Heat and electricity H 2 O (g) + CO 2(g) �� O 2(g) + H 2(g) + CO (g) Hydrogen, syn-gas and electricity co- � generation using non-CO 2 resources; promising route to decrease CO 2 -emissions, and enable large-scale energy storage. Large incentive for a reversible high- � temperature electrolysis-fuel cell (HTE-FC). GWs of gas turbines operate at few hundred � hours per year to meet peak electricity Stoots et al., demand (very expensive gas turbine). J. Fuel Cell Sci. � HTE-FC may be much more economic than Tech. 2009 HTE because of load following capability. 2

  3. Research approach in Laboratory for Electrochemical Interfaces ( lead by Prof. Bilge Yildiz, http://web.mit.edu/yildizgroup ) Isolate key parameters and unit processes using model systems in reaching to surface structure and chemistry in harsh environments. Surface chemical and electronic structure, laterally averaged; X-ray and Electron spectroscopies Surface electronic structure Electronic structure, cation- spatially resolved: oxygen bonding, reaction Scanning Tunneling and transport kinetics O 2 , H 2 , H 2 S… Microscopy/Spectroscopy First principles-based and O - (STM/STS) atomistic simulations e - Cathode Electrolyte GOAL: Understand the electronic and chemical behavior on oxide surfaces for energy applications: fuel cells, corrosion. 3

  4. STM / STS set-up and experiment conditions XPS STM /nc ‐ AFM Gas doser; Omicron VT ‐ 25 oxyge, hydrogen T = 500 o C Surface cleaning P O2 = 10 -5 mbar conditions t = 20-30 min Measurement T = 23 – 580 o C conditions P surface ~ 10 -3 mbar. (example for SOFC (Tested up to 20 mbar, 500 o C.) application) 4

  5. Example: Effect of strain in oxygen conductivity in Y 2 O 3 stabilized ZrO 2 (Electrolyte for SOFC/SOEC) Oxygen plane Oxygen plane 10 6 10 6 Oxygen ‐ Cation (O ‐ C) Oxygen ‐ Cation (O ‐ C) Cation (Zr,Y) Cation (Zr,Y) 1000 K 1000 K 10 5 10 5 bonding plane bonding plane 10 4 10 4 800 K 800 K 0 0 D O / D O D O / D O 600 K 600 K 10 3 10 3 Vacancy Vacancy critical critical 10 2 10 2 strain strain Decrease at higher Decrease at higher Increase up to a critical Increase up to a critical 400 K 400 K strains; strains; strain ( fastest strain ); strain ( fastest strain ); 10 1 10 1 Local relaxations, Local relaxations, Migration space, Migration space, 10 0 10 0 O ‐ C bond weakening. O ‐ C bond weakening. O ‐ C bond strengths. O ‐ C bond strengths. 0 0 0.02 0.02 0.04 0.04 0.06 0.06 0.08 0.08 Tensile strain Tensile strain The maximum relative enhancement in oxygen diffusivity ( D o /D o 0 ): 6.8 × 10 3 times at 4% strain at 400 K. Kushima A, Yildiz B: Oxygen ion diffusivity in strained yttria stabilized zirconia: where is the fastest strain? Journal of Materials Chemistry 2010, 20(23): 4809-4819. 5

  6. Example: In situ characterization of surface chemistry and electronic structure �� reactivity � La0.7Sr0.7MnO3 (LSM) � oxygen electrode for SOFC/SOEC Tunneling Current (nA) 0.6 C A B 0.3 0.0 RT, 10 ‐ 10 mbar -0.3 500° C, 10 ‐ 3 mbar -0.6 500 ° C, 10 ‐ 10 mbar 200x200nm 2 800x800nm 2 -2 -1 0 1 2 Tunneling at 2 V, 1 nA Bias Voltage (V) (A) Polycrystalline La 0.7 Sr 0.7 MnO 3 (LSM) thin film surface. (B) Step height-resolution (3.9 ± 0.2 Å) on the epixatial (100) LSM surface, at 580 o C, 10 -3 mbar. (C) PO 2 -dependence of the electron tunneling at 500 o C, on (B). Katsiev K, Yildiz B, Balasubramaniam K, Salvador PA: Electron tunneling characteristics on La0.7Sr0.3MnO3 thin-film surfaces at high temperature. Appl Phys Lett 2009, 95(9), 2009 6

  7. Example: Degradation of HTE materials Anode Poor adhesion Good adhesion 1 SSZ 3 Anode + 2 Bond Layer Bond Layer 4 10 μ m 200 μ m 20.0 µm ⎯ Mn, from the IC coating LSC Small amount of Cr Cr Sr Co • Cr poisoning • Cation / phase separation O = e - Anode Sharma VI, Yildiz B: Degradation Mechanism in La0.8Sr0.2CoO3 as SSZ Contact Layer on the Solid Oxide Electrolysis Cell Anode, Journal of The Electrochemical Society , 157, B441-B448, 2010 7

  8. Potential project objective in this program � To identify electrode compositions that are active and durable in reversible operation of solid oxide fuel cell (SOFC) / electrolysis cell (SOEC) � Synthesize thin model films, � Electrochemical performance characterization � Correlation of electrochemical performance (activity AND durability) to surface chemistry and electronic structure. 8

  9. University of Cambridge Atomistic Simulation Group � Background • Current Energy ‐ Related Projects • Fast ion conduction Group Leader in doped nanoscale STO ‐ YSZ Dr Paul Bristowe zirconia interface � Expertise: applied materials modeling using both classical MD and DFT � Member: UK consortium on first principles • Carbon capture in calculations (UKCP) metal ‐ organic Znbpetpa � User/developer: CASTEP DFT code framework unit cell � Energy ‐ related industrial collaborations: compounds Pilkington Glass , Philips Electronics , Osram Semiconductor s, Fiat , Bekaert Coatings • Doping mechanisms in oxide materials for � Former MIT researcher & visiting professor solar cells, sensors and displays Department of Materials Science and Metallurgy 9

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