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ORNL-1771 - Oak Ridge National Laboratory

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ANP QUARTERLY PROGRESS REPORT<br />

A161 SfATTERlNG OF NEUTRONS<br />

In an effort to understand the air-scattered neutron<br />

intensities which have been measured at the Tower<br />

Shielding Facility, a number of calculations have<br />

been carried out with a variety of conditions and<br />

assumptions. The predominant difference between<br />

the current work and that which WQS done pre-<br />

viously4 is that the interference of the ground has<br />

been taken into account. The ground Scattering is<br />

calculated separately. In an attempt to obtain a<br />

better fit to thc data, such aspects as anisotropy of<br />

scattering and slant penetration at the detector tank<br />

(crew shield) have been taken into account in some<br />

of the work. Furthermore, measurements have been<br />

made of the ongular distribution of the radiation<br />

leaving the reactor shield, and these data have<br />

been used i ~? some of the calculations.<br />

Because the importance of the multiply scattered<br />

neutrons has oppeared to be greater than was antici-<br />

pated, considerable effort lins been made to extend<br />

the calculations to beyond the singly scattered<br />

case. Some results are reported far two scatterings,<br />

and a general method has been developed for all<br />

orders of scattering.<br />

Single Anisotropic Air Scattering in the Presence<br />

of the Ground (Shielded Detectcab<br />

F. H. Murray<br />

For a convenient machine cnlculation, the at-<br />

tenuation in air WQS neglected. The detector was<br />

placed with 10 cm of water between it and the face<br />

of the crew shield which, when extended, contained<br />

the reactor source. The beam from the source was<br />

about an axis through the detector, in theory, and<br />

contained teinis cos a and cos2 q c1 calculation<br />

WQS made separately for the terms 1, cos 4 and<br />

cos2 a in i~ie expansion of the source flux. If D is<br />

the reactor-detector distance and h the height of<br />

both above the g~ound, the flux at the detector is<br />

expressed as the sum of the terms:<br />

and<br />

158<br />

where<br />

g(a + /3) = 1 + 0.3 cos (a t /3) I<br />

/(a) = a, 1; b, cos a; c, cos2 a .<br />

The angle + is the angle between the vertical<br />

plane taken as the face of the crew compartment<br />

and the plane triangle formed by the source, the<br />

scattering volume, and the detector, The results<br />

of this calculation5 will be published later.<br />

Single !sotrapis Air Scattering in the Presence<br />

of the Ground (Unshielded Detector)<br />

J. E. Foulkner<br />

A calculation was made of the reading of an iso-<br />

tropic detector caused by first-scattered neutrons<br />

in air as the distance above the ground was varied.<br />

The following assumptions were made:<br />

1. The source and detector have the same alti-<br />

tude,<br />

2. The ground is an infinite plane,<br />

3. The source is isotropic.<br />

4. The scattering in air is isotropic.<br />

5. There is no energy degradation on air scatter-<br />

Ing.<br />

6. The attenuation is pure inverse square.<br />

With these assumptions the reading on the detector<br />

may be shown to he proportional to<br />

1<br />

D<br />

where D is the separation of source and detector,<br />

h is the altitude, and / may be expressed in closed<br />

4See, for example, H. Goldstein, Chop. 2.9, p 831, in<br />

Reactor Handbook, ed by J. F. Hogerton and R. C.<br />

Grass, Technical Information Service, AEC, 1953.<br />

5-<br />

I-. H. Murruy, Single Anisotropic Air Scattering of<br />

Neutrons in the Presence of the Ground (Shielded<br />

Detector), '<strong>ORNL</strong> CF-548-1041 (to be issued).<br />

for O 5 4 5 n/2,

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