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European Journal of Scientific Research - EuroJournals

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403 R. Y. Tamakloe, K. Singh and Clovis A. Linkous<br />

Figure 6: Voltage–Current characteristic <strong>of</strong> a fuel cell with PtxPt experimental fuel cell, Al/xxx/Al and<br />

Al/xxx/Cu conductors<br />

Voltage / V<br />

1.20<br />

1.00<br />

0.80<br />

0.60<br />

0.40<br />

0.20<br />

PtxPt, Al/xxx/Al, Al/xxx/Cu Characteristics<br />

0.00<br />

0.00 0.20 0.40 0.60 0.80 1.00 1.20<br />

Current / A<br />

PtxPt<br />

Al/xxx/Al FC<br />

Al/xxx/Cu FC<br />

Figure 7: Voltage–Current characteristic <strong>of</strong> a fuel cell with PtxPt experimental fuel cell, Al/xxx/Al and<br />

Al/xxx/Cu conductors<br />

Voltage/V<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

I-V Characteristics<br />

0<br />

0.00 0.20 0.40 0.60 0.80 1.00 1.20<br />

Current/A<br />

Al/xxx/Cu<br />

Al/xxx/Al<br />

Al/xxx/Ni/Sn<br />

Al/xxx/Steel<br />

PtxPt<br />

4.0. Discussion<br />

The current collectors can impact the current-voltage characteristic in several ways. If they are not<br />

highly electronically conductive, then they can contribute to the Ohmic resistance <strong>of</strong> the cell. Another<br />

issue is mass transport <strong>of</strong> the gaseous reactants, H2 and O2. In this type <strong>of</strong> cell design in particular, if<br />

the current collectors are not porous, they may block or at least restrict the flow <strong>of</strong> reactive gas through<br />

the gas diffusion electrode. This would contribute to the mass transport limiting current <strong>of</strong> the cell. In

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