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Figure 6. 8 is R photograph of t le<br />

bent cylindrical ducts in position in<br />

<strong>the</strong> Lid Tank Facility. There are 19,<br />

round, aluminum pipes in a hexagonal<br />

array. Each pipe has an outside<br />

diameter of 3 15/16 in. and 1/16-in.<br />

walls. The pipes have three straight<br />

sections 22 in. long connected with<br />

45-deg bends. In <strong>the</strong> plane of <strong>the</strong><br />

source plate, <strong>the</strong> centers of <strong>the</strong><br />

pipes define equilateral triangles<br />

wit,h sides 7.33 in. long. Since <strong>the</strong><br />

ducts lecve <strong>the</strong> source plate at an<br />

angle of 22.5 deg to <strong>the</strong> normal, <strong>the</strong><br />

array is not symmetrical about <strong>the</strong><br />

source axis. With this arrangement,<br />

<strong>the</strong> fractions of <strong>the</strong> total volume thnt<br />

are air, water, and aluminum are 26.6,<br />

71.8, and 1.6%, respectively,<br />

The radiation measurements around<br />

this array have been obtained in considerable<br />

detail. An analysis of <strong>the</strong><br />

results shows that <strong>the</strong> gamma dose can<br />

TABLE 6.2. SUMMARY OF ACTIVITIES<br />

SAMPLE NEUTRON SHIELD<br />

Cobalt<br />

M angane se<br />

None<br />

Boron cover<br />

None<br />

Boron cover<br />

None<br />

Boron cover<br />

Boron backing<br />

Boron cover<br />

Boron backing<br />

POSITION WATER AROLND DUCT<br />

Outlet Duct<br />

Eoron cover<br />

- __<br />

Side<br />

Borated<br />

-<br />

-1 1 an g ane se None<br />

No:-<br />

Inlet Duct<br />

End<br />

Side<br />

P1 ain<br />

Plain<br />

-_ __-- . - - - -<br />

End<br />

End<br />

Side<br />

Side<br />

End<br />

End<br />

End<br />

End<br />

Side<br />

PERIOD ENDING DECEMBER 10, 1952<br />

be accurately computed by considering<br />

<strong>the</strong> ducts and water to ].)e ahomogeneous<br />

shield of appropriately reduced density.<br />

The neutrons, however, stream through<br />

<strong>the</strong> ducts in sufficient numbers to<br />

increase <strong>the</strong> flux at <strong>the</strong> end to one or<br />

two orders of magni tude greater than<br />

that predicted on a reduced density<br />

basis. This is in accordance with <strong>the</strong><br />

duct <strong>the</strong>ory proposed by Simon and<br />

Clifford, that is, geometrical attenu-<br />

ation along <strong>the</strong> straight sections and<br />

inverse sine reflection at <strong>the</strong> bends.<br />

The design of this particular array is<br />

not optimum, since <strong>the</strong> att,enuation<br />

through <strong>the</strong> ducts is not high enough<br />

to exceed that through <strong>the</strong> equivalent<br />

amount of water. An optimum design<br />

might. have ano<strong>the</strong>r bend in <strong>the</strong> ducts<br />

to increase <strong>the</strong>ir attenuation, or<br />

closer spacing between ducts to fur<strong>the</strong>r<br />

reduce <strong>the</strong> density of <strong>the</strong> equivalent<br />

homogeneous shield.<br />

INDUCED IN THE LID TANK FACILITY<br />

Borated<br />

Borated<br />

Borated<br />

Borated<br />

Plain<br />

Plain<br />

Borated<br />

Borated<br />

Borated<br />

I___-<br />

-I_<br />

ACTIVITY INDUCED<br />

( mc/ g)<br />

58.1 i 9.6 X 10"'<br />

5.5 f 9.1 X lo-''<br />

138.3 f 10.1 X<br />

18.3 f 9.3 X IO"'<br />

178.5 f 1.5 X<br />

4.64 f 0.17 X lom8<br />

68.3 f 1.0 X<br />

3.16 f 0. 16 X<br />

124.3 f 0.8 X<br />

11.7 i 0.3 X lo'*<br />

1.04 t 0.15 x 10'<br />

2.57 f 0.02 x 10'~<br />

77

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