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Inorganic Microporous Membranes for Gas Separation in Fossil Fuel ...

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2 Theoretical background<br />

pO2′′<br />

RT<br />

j = − ∫ t σ d ln pO<br />

(2)<br />

O2 2 e ion<br />

16F<br />

L pO2′<br />

2<br />

Thus, the oxygen flux (jO2) through dense ceramic membranes is dependent on the<br />

temperature (T), thickness (L), the electronic conductivity (σe; te= σe/[σe+σion]) and ionic<br />

conductivity (σion) of the membrane material and the oxygen partial pressure gradient<br />

(∆pO2) over the membrane. 16<br />

pO’2<br />

e<br />

A<br />

O 2-<br />

A B<br />

pO’’2<br />

10<br />

pO’2<br />

O 2-<br />

pO’’2<br />

Figure 2 Dense membrane concepts. A): oxygen pump. b): Mixed ionic and electronic conductor 16 .<br />

The most promis<strong>in</strong>g materials <strong>for</strong> oxygen separation and methane re<strong>for</strong>m<strong>in</strong>g membranes<br />

are the acceptor-doped perovskite-type oxides with the general <strong>for</strong>mula La1-xAxByO3-δ<br />

(A = Sr, Ba and B = Fe, Cu, Ni, Cr, Co). These compounds show high electronic and<br />

ionic conductivity. The highest oxygen flux has been obta<strong>in</strong>ed by Vente et al. 17,18 <strong>for</strong> a<br />

strontium barium iron doped cobaltate at 900˚C, see Table 2. The highest oxygen flux<br />

found <strong>in</strong> literature has been obta<strong>in</strong>ed with an oxygen partial pressure at the feed side of<br />

1 bar and a membrane thickness of only 0.2 mm, whereas the other results are based on<br />

membranes thicker than 1 mm. If the oxygen flux is normalised by the thickness than<br />

Mert<strong>in</strong>s et al. 19 measured the highest oxygen flux with atmospheric air at the feed side.<br />

The flux of the membrane reported by Mert<strong>in</strong>s et al. 19 is obta<strong>in</strong>ed by us<strong>in</strong>g methane as a<br />

sweep gas <strong>in</strong> comb<strong>in</strong>ation with a Ni-catalyst <strong>for</strong> methane re<strong>for</strong>m<strong>in</strong>g application.<br />

Decreas<strong>in</strong>g the thickness would improve the bulk diffusion. The oxygen transport will be<br />

rate determ<strong>in</strong>ed by the oxygen surface exchange 20 <strong>for</strong> membranes with a thickness less<br />

than 500 µm. Th<strong>in</strong> La1-xSrxCo1-yFeyO3-δ films supported on tailored ceramic substrates<br />

can be prepared 21 . Fluxes between 1 and 30 ml/cm 2 ·m<strong>in</strong> can be expected. 7<br />

2e -

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