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ORNL-5388 - the Molten Salt Energy Technologies Web Site

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A 12<br />

Table A-2. O<strong>the</strong>r Isotope Separation <strong>Technologies</strong><br />

~~ ~~ ~<br />

A. Discarded <strong>Technologies</strong><br />

Thermal Diffusion<br />

Electromagnetic (<strong>the</strong> Calutron Process)<br />

B. Developing <strong>Technologies</strong><br />

Photo-Exci tation Methods (Laser)<br />

Chemical Exchange Methods<br />

Aerodynamic Methods (O<strong>the</strong>r Than <strong>the</strong> Becker Nozzle<br />

and <strong>the</strong> Fixed Wall Centrifuge)<br />

P1 asma Based Processes<br />

The discarded technologies listed in Table A-2 have been used to produce<br />

enriched uranium.<br />

A large-scale, liquid-phase, <strong>the</strong>rmal-diffusion plant was constructed in 1945<br />

by <strong>the</strong> Manhattan Project.14 This plant produced very slightly enriched uranium<br />

(0.86%). Thermal diffusion is impractical for commercial enrichment of uranium<br />

isotopes because of its very high energy requirements. Compared to gaseous diffusion,<br />

<strong>the</strong> energy requirement is over 200 times greater.<br />

The electromagnetic or Calutron methods were used during <strong>the</strong> Manhattan Project<br />

to produce highly enriched uranium. 14 The process was discarded shortly after <strong>the</strong><br />

more economical gaseous diffusion plant began ,operation. A brief description of <strong>the</strong><br />

process follows.<br />

The Calutron Process involved <strong>the</strong> vaporization of a salt feed material,<br />

typically UC14, from an electrically heated charge bottle through slots into an arc<br />

chamber where <strong>the</strong> salt was ionized by an electron beam which travels along <strong>the</strong> lines<br />

of flux of <strong>the</strong> magnet. The ionized uranium, as <strong>the</strong> U+ ion for <strong>the</strong> most part, passed<br />

through ano<strong>the</strong>r slot where it was accelerated by o<strong>the</strong>r slotted electrodes into <strong>the</strong><br />

vacuum tank which filled <strong>the</strong> pole area of a large electromagnet. The ions from <strong>the</strong><br />

accelerating electrodes diverged several degrees from <strong>the</strong> slots and at <strong>the</strong> 90" point<br />

passed by some baffles as a ra<strong>the</strong>r thick beam. This beam was brought to a focus at <strong>the</strong><br />

slots of a receiver system as curved lines by <strong>the</strong> shimmed magnetic field. In <strong>the</strong><br />

large units, 96-in. beam diameter, <strong>the</strong>re were up to four of <strong>the</strong>se beams in a given<br />

tank. The divergent trajectories of <strong>the</strong> ions from <strong>the</strong> four sources intersected some<br />

few degrees from <strong>the</strong> accelerating electrodes and separated as distinct beams, again a<br />

similar distance from <strong>the</strong> receivers. There were various side beams of UCl', U++, and<br />

o<strong>the</strong>r ions which hit <strong>the</strong> baffles and <strong>the</strong> walls of <strong>the</strong> tank at a series of locations.<br />

The uranium content of <strong>the</strong>se beams condensed as various compounds of uranium. The<br />

product was, for <strong>the</strong> most part, converted to UC by interaction of <strong>the</strong> very high<br />

voltage uranium ions with <strong>the</strong> graphite of <strong>the</strong> receivers. Since, in even <strong>the</strong> most<br />

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