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ORNL-1816 - the Molten Salt Energy Technologies Web Site

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ANP QUARTERLY PROGRESS REPORT<br />

In calculating <strong>the</strong> activity of <strong>the</strong> fission frag-<br />

ments, use is made of Fig. 2 in <strong>ORNL</strong>-53,6 which<br />

is a curve of <strong>the</strong> dose from a uranium slug exposed<br />

for three years plotted against time after exposure.<br />

The dose is given in mrhr at 1 meter per watt of<br />

exposure,<br />

Calculations now show that 1 curie of 2-Mev<br />

gammos gives a dose of approximately 1 rhr at<br />

1 meter. If it is assumed that <strong>the</strong> average energy<br />

of <strong>the</strong> decay gammas from <strong>the</strong> fission fragments<br />

is 2 Mev (an overestimate), <strong>the</strong> curve can be used<br />

to obtain an estimate of <strong>the</strong> curies of activity for<br />

c?y time after exposure. However, it is first<br />

necessary to calculate <strong>the</strong> watts of exposure in<br />

<strong>the</strong> regions of <strong>the</strong> reactor close enough to <strong>the</strong><br />

lnconel core shells so that <strong>the</strong> fragments due to<br />

fissions will strike <strong>the</strong> Inconel. This is done by<br />

finding <strong>the</strong> range, R, of <strong>the</strong> fission fragments in<br />

<strong>the</strong> fuel and again approximating <strong>the</strong> fuel annulus<br />

by a spherical shell of 25 cm OD and 15 cm ID<br />

to find <strong>the</strong> total power generated in <strong>the</strong> regions<br />

adjacent to <strong>the</strong> Inconel. This power is divided<br />

by 2 to account for <strong>the</strong> fact that approximately<br />

one-half <strong>the</strong> fission fragments generated in this<br />

region will impinge on <strong>the</strong> shells. Since <strong>the</strong> curve<br />

was plotted for a slug exposed for three years,<br />

any values obtained by using this curve will be<br />

overestimates of <strong>the</strong> fission fragment activity of<br />

a 60-Mw reflector-moderated reactor,<br />

The range of fission fragments is estimated to<br />

be 0.001 cm, and <strong>the</strong><br />

1<br />

watts of exposure = 6 x lo7 w x -<br />

2<br />

4n (252 + 152) x<br />

X x 2<br />

4<br />

- r7 (253 - 153)<br />

3<br />

= 1.3 io4 .<br />

6G. Ascoli and 0. Sisman, Absorption o Radiation<br />

from an "X" Slug by Lead, Fig. 2, p 7, ORAL-53 (May<br />

1948).<br />

28<br />

The last factor of 2 in <strong>the</strong> above equation is due<br />

to <strong>the</strong> flux at <strong>the</strong> surface of <strong>the</strong> lnconel being<br />

twice that of <strong>the</strong> average flux. Some values of<br />

<strong>the</strong> total activation of <strong>the</strong> lnconel core shells<br />

obtained by using <strong>the</strong> above methods are given in<br />

Table 2.1. One conclusion to be drawn from<br />

Table 2.1 is that little would be gained by trying<br />

to obtain special lnconel with especially low<br />

cobalt content; <strong>the</strong> activity could not be reduced<br />

below that caused by <strong>the</strong> fission fragments.<br />

TABLE 2.1. ACTIVATION OF INCONEL<br />

CORE SHELLS<br />

Activity (curies)<br />

Days After<br />

Fission<br />

Exposure Cobalt<br />

Fragments<br />

Total<br />

10 480 390 870<br />

20 480 260 740<br />

100 480 80 560<br />

Ma<strong>the</strong>matical Models for Reflector-Moderated<br />

Reactors<br />

L. T. Anderson, Consultant<br />

The <strong>the</strong>rmal absorption rate has been calculated<br />

for an idealized reactor consisting of a nonmoder-<br />

ating spherical-shell fuel region surrounding a<br />

moderator and surrounded by an infinite moderating<br />

reflector with a fission source of 1 neutrodsec<br />

in <strong>the</strong> fuel region. The <strong>the</strong>rmal capture cross<br />

section of <strong>the</strong> fuel region was taken to be infinite.<br />

The non<strong>the</strong>rmal capture cross section of <strong>the</strong> fuel<br />

region was assumed to be zero, and <strong>the</strong> <strong>the</strong>rmal<br />

and non<strong>the</strong>rmal absorption cross sections of <strong>the</strong><br />

moderator were likewise assumed to be infinitely<br />

small. The neutrons slowed down according to age<br />

<strong>the</strong>ory, and <strong>the</strong> <strong>the</strong>rmal neutrons diffused according<br />

to diffusion <strong>the</strong>ory.<br />

The absorption rate is, for <strong>the</strong> source located at<br />

<strong>the</strong> inner<br />

(2<br />

radius of <strong>the</strong> fuel region,<br />

1 + - 1) x cotx

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