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ORNL-1816 - the Molten Salt Energy Technologies Web Site

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ANP QUARTERLY PROGRESS REPORT<br />

In conclusion it can be said that at <strong>the</strong> 200-ft<br />

altitude <strong>the</strong> ground-scattered contributions to air-<br />

scattering experiments at <strong>the</strong> TSF are dependent<br />

IO<br />

2- c 3<br />

5<br />

e<br />

e<br />

-D<br />

2<br />

-<br />

-<br />

X I<br />

3<br />

LL J<br />

z 05<br />

$<br />

!- 3<br />

2 02<br />

J 4<br />

5 01<br />

W<br />

I !-<br />

yo05<br />

-<br />

5<br />

L 002<br />

0 01 0 40 80 (20 160 200<br />

h. REACTOR-DETECTOR ALTITUDE (ftl<br />

Fig. 12.10. Comparison of Scattered-Neutron<br />

Calculations with Preliminary Differential Experi-<br />

ment.<br />

150<br />

on <strong>the</strong> source geometry; however, <strong>the</strong> contributions<br />

will be small, that is, not more than 5%, in all<br />

cases.<br />

10<br />

- 5<br />

* -<br />

c<br />

h<br />

E- 2<br />

-D<br />

-<br />

X I<br />

3 LL<br />

z 05<br />

8<br />

c 3<br />

Y 02<br />

1<br />

a<br />

8 01<br />

I<br />

+<br />

5<br />

W 005<br />

W<br />

[L 002<br />

spem?l<br />

2-01-056-3-T22<br />

0 01 0 20 40 60 80 100 120 140 160 180 200<br />

h, REACTOR-DETECTOR ALTITUDE (ft)<br />

Fig. 12.11. Comparison of Scattered-Neutron<br />

Calculations with GE-ANP R-1 Mockup Experiment.<br />

7<br />

P<br />

i

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