The gas permeability measurements were performed using a stainless-steel cell with two identical chambers separated by the film. The permeability was evaluated by pressurising the feed chamber up to 0.7 bar with pure gas, namely carbon dioxide (99.998%) or oxygen (99.999%) (Praxair, Maia, Portugal), followed by the measurement of the pressure change in both chambers over time, using pressure transducers (JUMO, Model 404327, Fulda, Germany). The temperature was maintained at 30 °C using a thermostatic bath (Julabo, Model EH, Seelbach, Germany). The permeability was calculated using Equation (6):
where Δp (bar) is the pressure difference between the feed and permeate compartment, P (m−2 s−1, where 1 barrer = 1 × 10−10 cm3 (STP) cm cm−2 s−1 cm Hg−1 = 8.3 × 10−13 m2 s−1) is the gas permeability, t (s) is the time, δ (m) is the film thickness, and β (m−1) is the geometric parameter of the cell, as described by Ferreira et al. [2].
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