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ORNL-5388 - the Molten Salt Energy Technologies Web Site

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3-6<br />

3.1. ESTIMATED U CONCENTRATIONS IN DENATURED U FUELS<br />

D. T. Ingersoll<br />

Oak Ridge National Laboratory<br />

Although it is mandatory that’<strong>the</strong> concentrations of 232U at each stage of <strong>the</strong> fuel<br />

cycle be predictable for <strong>the</strong> various reactors operating on thorium-based fuels, little<br />

information on <strong>the</strong> subject is available at this time. This is attributable to <strong>the</strong> fact<br />

that <strong>the</strong> interest in thorium fuel cycles is relatively recent and <strong>the</strong>refore <strong>the</strong> nuclear<br />

data required for calculating <strong>the</strong> production of 232U have not been adequately developed.<br />

Of primary importance are <strong>the</strong> (n,y) cross sections of 23’Pa, 230Th, and 232Th and <strong>the</strong><br />

(n,Zn) cross sections of 233U and 232Th, all of which are intermediate interactions that<br />

can lead to <strong>the</strong> formation of 232U as is illustrated by <strong>the</strong> reaction chain given in Fig.<br />

3.1-1.<br />

These cross sections are under current evaluation’ and should appear in <strong>the</strong> Version<br />

V release of <strong>the</strong> Evaluated Nuclear Data File (ENDF/B-V).<br />

I<br />

232<br />

9oTh<br />

I<br />

h2n)<br />

t<br />

E h l<br />

Fig. 3.1-1 Important Reaction Chains<br />

Leading to <strong>the</strong> Production of 232U.<br />

3.1.1. Light-water Reactor Fuels<br />

In spite of <strong>the</strong> nuclear data deficien-<br />

cies, some results for 2321) concentrations<br />

are available from calculations for denatured<br />

fuels in light-water reactors (LWRs) and in<br />

fast breeder reactors (FBRs) . A1 though no<br />

results for denatured high-temperature gas-<br />

cooled reactors (HTGRs) are currently available,<br />

232U concentrations can be roughly inferred<br />

from existing HTGR fuel data. Moreover, <strong>the</strong><br />

analysis of 232U concentrations in standard<br />

HTGR designs (HEU/Th) serves as an upper<br />

bound for <strong>the</strong> denatured systems.<br />

tion of <strong>the</strong> available results is given below.<br />

The current state of <strong>the</strong> related 232U nuclear<br />

data is amply reflected in <strong>the</strong> large variances<br />

of <strong>the</strong> calculated concentrations.<br />

A compila-<br />

Existing data on 232U concentrations in denatured LWR fuels are primarily from cal-<br />

culations based on <strong>the</strong> Combustion Engineering System 80TM reactor design.2 Results from t ’<br />

CE3 for a denatured 235U cycle (20% 235U-enriched uranium in 78% thorium) show <strong>the</strong> 232U L<br />

concentration after <strong>the</strong> zeroth generation to be 146 ppm 232U in uranium, while after<br />

five generations of recycle uranium, <strong>the</strong> concentration is increased to 251 ppm.<br />

levels are in good agreement with <strong>ORNL</strong> calculation^,^ which indicate 130 ppm 232U in<br />

uranium for <strong>the</strong> zeroth generation. The discharge uranium isotopics are summarized in<br />

Table 3.1-1.<br />

These<br />

Also shown are <strong>the</strong> results from an <strong>ORNL</strong> calculation for a denatured 233U cycle<br />

L<br />

L; h

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