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3.4. U-Tube Hydriding Reactor<br />
The U-tube that was used for scaled up experiments was filled with approximately<br />
190 grams of LaNi 5 and then the flow of 2% (v/v) H 2 :He at about 9 atm was fed into it.<br />
The flow out of the reactor was restricted to about 200 mL.min -1 by a pressure relief<br />
valve. The valve maintained the pressure within the reactor, while allowing a slow flow.<br />
The gas chromatogram of multiple injections is given in Figure 35. The single peaks over<br />
the first 20 minutes were helium peaks, represented by empty circles. Hydrogen was not<br />
observed in the effluent because it reacted with LaNi 5 . When LaNi 5 could not absorb any<br />
more H 2 , hydrogen peaks started to show (filled circles). The percent hydrogen values in<br />
the effluent were calculated using peak area ratios of H 2 and He. The breakthrough curve<br />
was plotted as a function of time (Figure 36).<br />
The U-tube reactor successfully removed the hydrogen from the H 2 -He stream<br />
and allowed the passage of He only. The amount of hydrogen retained in the reactor at<br />
the time of saturation was calculated from material balance. The amount of helium<br />
leaving the system was calculated using flowrate and time<br />
V He (mL) = flowrate (mL.min -1 ) x time (min)<br />
which was equal to the amount of He that entered the system. Since the composition of<br />
the entering gas mixture was known, the amount of H 2 entered was calculated using<br />
V Hydrogen = V He x (20/80)<br />
and converted to the amount and then weight percent hydrogen in the LaNi 5 .<br />
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