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PLENTIFUL ENERGY

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The first thing we wish to know is the state of saturation of the cadmium. In<br />

these experiments the cathode contained 26 kg of cadmium. The number of moles<br />

of cadmium were 26000/112.4 = 232 moles. Uranium saturates at a concentration<br />

of 1.12%, 0.0112 x 232 = 2.60 moles U, or 2.6 x 238 = 618.8 grams U. Plutonium<br />

saturates at a concentration of 1.81% = 0.0181 x 232 = 4.20 moles Pu, or 4.2 x 239<br />

=1003.8 grams Pu. Thus the saturated amounts of the metals in the cadmium<br />

cathode are 618.8 grams U and 1003.8 grams of Pu.<br />

The anode in all three runs was EBR-II blanket material, substantially uranium,<br />

only 1 percent or so was plutonium. The effect of this anode composition is to<br />

increase the uranium content in the electrolyte as cadmium cathode electrorefining<br />

proceeds. Uranium largely replaces plutonium in the electrolyte reduced at the<br />

cathode. The measured results are given in Table A-5.<br />

Table A-5. Results of Transuranic Recovery Experiments<br />

Run 1 Run 2 Run 3<br />

Heavy metal recovered, g 1365 1739 1313<br />

Pu in casting furnace ingot, g 1024 1080 492<br />

Np-237 in casting furnace ingot, g 4.5 1.2 0.6<br />

U in salt at end of test, wt% 0.47 0.74 0.83<br />

Pu in salt at end of test, wt% 2.67 2.46 2.38<br />

Recovered metal theoretical, 10 6 coulomb 1.65 2.11 1.59<br />

Integrated current, 10 6 coulomb 1.81 2.13 2.09<br />

Transport efficiency, % 91.5 99.2 76.1<br />

A.12.3 Equilibrium Constants Derived From the Measured Quantities<br />

of Each Run<br />

Our reaction is Pu + UCl 3 U + PuCl 3 .<br />

Our calculated value for the equilibrium constant for the reaction is fixed at<br />

1.2x10 6 , unchanged from run to run. We will compare this to the values derived<br />

from the measured results of the three electrorefining runs. We want to see how<br />

well calculations based on the assumptions we use, principally that of equilibrium,<br />

are able to predict results.<br />

The required input data is shown in Table A-6 below. We are indebted to Dee<br />

Vaden of INL for explanation of the details of the experiments, published in<br />

378

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