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hydrogen production from water using solar cells powered nafion ...

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Figure 4.2. Pin Type Flow Field<br />

Except the flow field design, the rest of the materials used in the second design<br />

were the same as the first one. The cell was tested under the same conditions and it was<br />

observed that the required potential difference decreased to 3.08V at 200mAmp/cm 2 which<br />

is 38.4% lower than that obtained in the first design. But the voltage efficiency of the cell<br />

was still about 48% even at this low current density. During this test, it was noticed that as<br />

the bolts getting tighter, voltage of the cell decreased continuously. In fact, 5mm<br />

polypropylene bolts could not be tightened more because they could be broken or lose<br />

threads.<br />

These tests showed the effect of compression on electrolysis cell that resulted in<br />

<strong>using</strong> thicker bolts with big thread sizes on further trial which tolerated high compression.<br />

6mm polypropylene bolts with big thread were used in the third experiment with all the<br />

other materials were the same as the second design. At the same temperature and <strong>water</strong><br />

flow rate, the potential difference decreased to 2.77V at 200mAmp/cm 2 which was 10%<br />

lower than that of the second design but still too high for such low current densities<br />

according to the results in the literature which were given in chapter two. At the end of the<br />

experiment, the cell was dismantled and similar to the X type flow field observations with<br />

the first design, the surface of the GDL was not as flat as that in the beginning of the test.<br />

On the surface of GDL, the points above the pins were little higher than the areas which<br />

were not supported by the pins. Since the deep fields on the GDL cannot contact with<br />

44

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