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ORNL-4191 - the Molten Salt Energy Technologies Web Site

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133<br />

Table 9.9. Comparison of Aqueous Chelotiny Agent with HN03 Leach for Removing Geposited<br />

Fission Products from Graphite and Hastelloy<br />

._.._._. __I..._ ~... .__. .<br />

Disintegrations per<br />

Exposed<br />

Minute in Total Sanrple<br />

Samplea<br />

in - 9 9 ~ ~ 0 132TC. 103Ru 95%,<br />

Gas CGB V<br />

A<br />

T<br />

Liquid CGB V<br />

A<br />

T<br />

Go s Hastelloy N V<br />

A<br />

T<br />

Liquid Hastelloy N V<br />

A<br />

T<br />

x 10'O<br />

4.6<br />

1.7.5<br />

6.35<br />

4.60<br />

3.24<br />

7.84<br />

4.65<br />

0.21<br />

4.87<br />

2.24<br />

1.51<br />

3.75<br />

% 1o'O<br />

2.99<br />

32.1<br />

35.1<br />

2.99<br />

2.25<br />

5.24<br />

5.89<br />

70.2<br />

76.1<br />

1.99<br />

15.5<br />

17.5<br />

x io9<br />

0.15<br />

1.19<br />

1.34<br />

0.154<br />

3.00<br />

3.15<br />

0.12<br />

0.07<br />

0.66<br />

0.73<br />

*V represents leaching in aqueous chelating solution; A represents leaching in acid; T represents total,<br />

Since this solvent dissolves salts but not<br />

metals, <strong>the</strong>se observations may possibly indicate<br />

that 99M0 and "Nb are present as oxidized<br />

species (fluorides?), while tellurium and tu<strong>the</strong>nium<br />

are present as metals. Wiping with a<br />

cloth removed larger fractions of 'OM0 and "Nb<br />

than of activities such as '32Tt?, I3'I, y5Zr,<br />

I4'Ba, and 89Sr which penetrated <strong>the</strong> graphite.<br />

The depmition of fission products on pyrolytic<br />

graphite (see Table 9.10) in <strong>the</strong> gas phase was<br />

similar to that on CGB graphite, although 132Te<br />

deposited to a smaller extent on <strong>the</strong> pyrolytic<br />

graphite. In <strong>the</strong> liquid phase, 9yM0 and '"Te<br />

deposited slightly more heavily on pyrolytic<br />

graphite than on <strong>the</strong> CGB.<br />

The deposition of "Nb was markedly heavier<br />

on Hastelloy N in <strong>the</strong> liquid phase than in <strong>the</strong> gas<br />

phase. Tellurium-132 and '"Ha deposited more<br />

heavily on <strong>the</strong> metal exposed in <strong>the</strong> gas phase.<br />

O<strong>the</strong>r isotopes deposited similarly on metal in<br />

<strong>the</strong> two environments.<br />

When metal and graphite were exposed to <strong>the</strong><br />

gas phase, somewhat mote '32Te, I3'I, arid<br />

95Zr deposited on <strong>the</strong> metal. When both were<br />

exposed to <strong>the</strong> liquid phase, less "Mo, 14'Ra,<br />

and 89Sr and more 'j2Te and 13LI deposited on<br />

<strong>the</strong> Hastelloy. The deposition per square centimeter<br />

of R given isotope varied by less than a<br />

x 10'<br />

4.3<br />

0.89<br />

5.23<br />

0.13<br />

4.47<br />

1.49<br />

, 3.5 for 1"3R~, 14.0 for loiRu, 95 for<br />

95Nb, and 56 for "Zr. A similar comparison of<br />

<strong>the</strong> activities on <strong>the</strong> Hastelloy N specimens from<br />

<strong>the</strong> two exposures (Tables 9.6 and 9.10j J ves<br />

ratios of 20 for "Mo, 6 for '32Te, 170 for 103Ri~,<br />

400 for '*'IRU, 7.5 for "Nb, arid 30 for 9sZr. The<br />

ratio of full-power exposure times is 417; <strong>the</strong> ratio<br />

of total exposure times is, of course, considerably<br />

greater. Both sets of activity ratios may be biased<br />

high since <strong>the</strong> sample holder in <strong>the</strong> 8-hr exposute<br />

may have intercepted a sii;able fraction of<br />

<strong>the</strong> depositing activities.<br />

Examination of <strong>the</strong> ratios given above shows<br />

that only deposition of "'Ru 011 Hastelloy N<br />

proceeds at approximately <strong>the</strong> same rate for 8<br />

as for 3340 full-power hours. However, <strong>the</strong><br />

measured deposit of a given radioactive nuclide<br />

actually reflects <strong>the</strong> deposition rate only<br />

over <strong>the</strong> last two or three half-lives of exposure<br />

time for that nuclide. Thus <strong>the</strong> measured ac-

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