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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

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