European Journal of Scientific Research - EuroJournals
European Journal of Scientific Research - EuroJournals
European Journal of Scientific Research - EuroJournals
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Operating Characteristics <strong>of</strong> Proton-Exchange-Membrane (PEM) Fuel Cells 404<br />
fact, it may be <strong>of</strong> interest that Al/xxx/Cu cell did not clearly exhibit mass transport overpotential, while<br />
it was clearly observable for Al/xxx/Al cell. Finally, the collector may undergo galvanic reaction,<br />
oxidizing itself to provide external current. Compared to PtxPt fuel cell, the platinum electrodes are<br />
also acting as both catalyst and conductor, shown is Fig. 7.<br />
As an experimental variable, any gas leakage would lower the partial pressure <strong>of</strong> the gas at the<br />
electrode/electrolyte interface, hence lowering the current density. Actually, the current-voltage curves<br />
for the two fuel cell current collector combinations do not vary all that much; it is only at high currents<br />
that the Al/xxx/Al cell seemed to mass transport limit sooner. Corrosion <strong>of</strong> the anode current collector<br />
is a fundamental problem <strong>of</strong> fuel cell technology, and so was observed in this designed too. Corrosion<br />
<strong>of</strong> some materials may occur even without producing an external current, undergoing a redox reaction<br />
directly with water, O2, or the combination <strong>of</strong> the two. The anode assumes the potential given by the<br />
partial pressure <strong>of</strong> O2 over it, which at room temperature, open circuit, acidic standard state, and one<br />
atmosphere <strong>of</strong> pressure, is 1.23 V. Very few electronically conductive substances are indefinitely stable<br />
under those conditions.<br />
The reason for the initial drop (Fig. 7), or activation polarization, is probably due to effects <strong>of</strong><br />
internal resistance <strong>of</strong> conducting metals as there is no change in the electrode characteristics. This<br />
effect is also depicted by the dominant factor for the linear drop in the operating range adding to the<br />
ohmic resistance <strong>of</strong> the electrolyte.<br />
Table 3: Variation <strong>of</strong> efficiency with internal resistance<br />
Conductor Int Res/ohm Efficiency Efficiency %<br />
AlxxxSteel 0.016 0.061 6.0<br />
PtxxxPt 0.035 0.473 47.3<br />
AlxxxNi/Sn 0.043 0.216 21.6<br />
AlxxxCu 0.074 0.557 55.7<br />
AlxxxAl 0.076 0.554 55.4<br />
AlxxxSn 0.089 0.041 4.1<br />
Efficiency<br />
0.60<br />
0.50<br />
0.40<br />
0.30<br />
0.20<br />
0.10<br />
Figure 8: Variation <strong>of</strong> efficiency with internal resistance<br />
Al/xxx/Steel<br />
Resistive-Efficiency Characteristics<br />
PtxPt<br />
Al/xxx/Ni/S<br />
0.00<br />
0.00 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08 0.09 0.10<br />
Internal Resistance / ohm<br />
The current-voltage characteristics show that conductor characteristic play significant role in<br />
the fabrication <strong>of</strong> the fuel cell. Obviously electronically conductive materials contribute less ohmic<br />
resistance to the cell. In this type <strong>of</strong> cell design in particular, the current collectors are not porous, they<br />
Al/xxx/Cu<br />
Al/xxx/A<br />
l<br />
Al/xxx/Sn