RADIATION PROTECTION WITHIN A

THE SHORTER-TERM BIOLOGICAL HAZARDS OF A FALLOUT FIELD

$7] GAMMA RADIATION (MR/HR)

16

tb coNcRETE

LEVEL

GROUND

SLABS Topen PORGH

SECTION Am~A
Frieure 4.-—Section View,

speaker said seems to be quite correct, in that
surface roughness affects readings in this way.

Wehave observed that sometimes the reading

will rise to as large a height as 30 feet before
beginning to fall if the surface is rough enough.
The shape of the curves he showed seem to be
in agreement with our experimental and theo-

retical work.

Mr. Gravuson. This is approached by a
thick slab calculation, such as you get over
water, where the material is distributed in
depth, and then any slant distances are highly
preferentially absorbed and the source seems
to be almost a monodirectional plane source.
Mr. Hottann (AEC). On the other hand,
youhave an increase of something of the order
of 4 or 5 mr per hourin the indoor curve. It
seems as though this would haveto be reflected.

This would be added onto the doses outdoors

as you went up and would give you a departure

from the theoretical curve, wouldn'tit?
Mr. Graveson. I am sorry I didn’t quite

INSIDE

@+

QUTSIDE (OPEN FIELD)

STATION 4

STATION 3

4 STATION |

Th

true plane calculation.

Therefore, the irregu-

larities could not he serious to give this type of
result. The small irregularitics could, and itis

6.

possible did contribute.

gL

‘r

3}

r
0

follow what you meant by your question,

Would you rephrase it?
Mr. Houianp. I assume that the theoretical
, curve for the decrease of dose rate with height
does not include this effect of irregularities?
Mr. Graveson. It as such does not. It isa

[.

2

GAMMA

J

4

at

1

5

Qo

6

GAMMA

RADIATION (MR/HR)
VERTICAL

RADIATION

FIG-5
Figure 5.—Vertical Radiation Profile.

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\

15
RADIATION (MR/HR)
ite)

PROFILE

STANDARD HOUSING STRUCTURE

17

Mr. Hownann. If they were of the magnitude

shown which is of the order of several—I don’t

remember the exact magnitude-—many r per
hour increase, it seems to me they would have
shown up on that curve, and particularly since
those readings were taken indoors the same
effect would probably be larger if existed outdoors. In other words, I am trying to pointto
the other indication. There must have been
contamination on the roof.
Mr. Gravison. Onthe other hand,if we had

contamination on the roof, which would match

these readings, the contamination density
would have been 3 or § times higher than the
contamination density on the ground. I am
not in a very strong position here. J am just
saying I am presenting some measurements
whieh I think are verv interesting.
Dr. Werner. Are there any further comments on this?
Mr. Recuen (Publie Health Service). I have
a feeling on this that what was missing was 4
theoretical curve for the indoor type of measurement where you have an uncontaminated slab
under the measuring instrument.
Mr. Graveson. The theoretical curve we
derived was based on the simplest case, that of
a smooth plane. This neglected unevenness of
the surface. When the major radiation contributionis from outsidea clean area, this is not
applicable. The Theory for thick slab source
is under examination.

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