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To connect these stochastic processes and the deterministic ATM model, we used a hybrid simulation algorithm (see Materials and Methods and reference [22]).
Typical values of electronic conductivity measured for this material at 800 °C were about 0.37 S m−1 at Po2=10−16 atm and 0.58 S m−1 at PO2=10−18 atm.
Thermodynamic computations have confirmed the possibility of using CO as a sublimation activator for enhancing the sublimation rate of the feed material in a large range of pressures (10−3 to 1 atm) and temperatures (800 1200 °C).
More than anything, the hydrogen storage capacity of this material is about 4 mmol g−1 at 300 K and 1 atm.
A business plan produced by the Peel Regional Police in 2001 describes how the CBA provided material and operational support during an investigation into identity theft and ATM fraud in the region.
However, a lack of practical materials that could contain the corrosive reaction mixture at the high pressures needed (200 atm or more) discouraged commercialization of these routes.
Using this rationale we have produced materials able to store up to 1.7% (w/w) of H2 at 77 K and 1 atm with such high ultramicroporosity that the DOE-goal H2 densities established for 2010 could be complied at pressures well below 5 atm.
The performance of La0.85Sr0.15MnyO3 ± δ (LSMy) as cathode material for Solid Oxide Fuel Cells (SOFC) operating at 1000 °C and pO2 = 0.21 atm.
Conversely, highly enhanced densification and grain growth are achieved by firing the materials at reduced temperatures (800 < T < 1200 °C) in low oxygen activity atmospheres (pO2 < 10−12 atm).
This kind of carbon material showed a CO2 uptake of 4.3 mmol g−1 with high selectivity at 298 K under 1 atm [24].
A commercially available LaNi4.8Al0.2 intermetallic compound was chosen as hydrogen storage material, having sorption characteristics adequate to the working conditions of the system (i.e. 60 °C and 1 atm).
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