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ORNL-2106 - the Molten Salt Energy Technologies Web Site

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R<br />

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c<br />

.<br />

--.<br />

in. long, 18’4, in. wide, and 2% in, thick. The<br />

beryllium layer immediately below it was 34% in.<br />

long and 245/,, in. wide.<br />

The top layer and <strong>the</strong> corners of <strong>the</strong>,second<br />

beryllium layer were subsequently removed, and<br />

<strong>the</strong> resulting reflector was 8% in. thick. The<br />

new top layer was 18’) in. wide and 34% in.<br />

1 6.<br />

long, A second longitudinal traverse was <strong>the</strong>n<br />

made. The results are shown in Fig. 4.4.4, in<br />

which <strong>the</strong>.top lobe is plotted to a scale one-half<br />

that used to plot <strong>the</strong> end lobe.<br />

Two series of lateral traverses were also made<br />

at <strong>the</strong> side of <strong>the</strong> reactor at several distances<br />

from <strong>the</strong> mid-plane. For reflector thicknesses of<br />

118 and 8% in. <strong>the</strong> outer slab dimensions for<br />

each side reflector thickness were <strong>the</strong> same as<br />

those given above. The latitudinal variations of<br />

<strong>the</strong> fast-neutron leakage for <strong>the</strong> two reflector<br />

thicknesses are shown in Figs. 4.4.5 and 4.4.6.<br />

The curves show a slight asymmetry about <strong>the</strong><br />

center of <strong>the</strong> reactor, which is attributed to <strong>the</strong><br />

reflection of neutrons by <strong>the</strong> aluminum and steel<br />

structure on which <strong>the</strong> critical assembly rests.<br />

The area under each curve of Figs. 4.4.5 and<br />

4.4.6 is proportional to <strong>the</strong> counting rate observed<br />

at <strong>the</strong> corresponding distance from <strong>the</strong> mid-plane<br />

in <strong>the</strong> longitudinal traverses made at <strong>the</strong> top of<br />

<strong>the</strong> reactor. By integrating <strong>the</strong> results of <strong>the</strong> two<br />

longitudinal traverses over <strong>the</strong> distance from <strong>the</strong><br />

mid-plane, it was possible to determine that <strong>the</strong><br />

removal of <strong>the</strong> 2% in. layer of beryllium from <strong>the</strong><br />

top of <strong>the</strong> reactor increased <strong>the</strong> fast-neutron leak-<br />

age <strong>the</strong>re by a factor of 3.7.<br />

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$ 6<br />

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4<br />

-I W<br />

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0<br />

-<br />

PERIOD ENDfNG JUNE IO, 1956<br />

shmc<br />

<strong>ORNL</strong>-LR-DWG 44421<br />

MEASURED WITH 2- in.- DIA<br />

HORNYAK BUTTON<br />

TOP BERYLLIUM LAYER:<br />

48% x 34314 in.<br />

THE MTA AT THE TOP<br />

- OF THE REACTOR ARE<br />

PLOTTED TO A SCALE<br />

ONE-HALF THAT USE0<br />

FOR PLOT OF THE EN0<br />

Fig. 4.4.4. Polar Distribution of Fast-Neutron<br />

Leakage at Surface of 8kin.ofhick Reflector of<br />

Compact-Core Reflector-Moderated-Reactor Critical<br />

Assembly.<br />

259

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