the cloud before transport by winds)

and the diffusion rate off the cloud

as it was moved by the winds.*
The primary fallout plot technique initially used on CASTLE was a
joint analysis of the hodograph and the 72-hour airborne parti@le trajec-

tory forecast to define the fallout area for the first l2-hourfperiod and
assess the orientation and areal extent of the cloud after theffirst 12
hours.
tempted;

For BRAVO, the method of elliptical approximations was[first atits use was extremely limited, however, because of undertainties

in its application to high-yield events.

The BRAVO data were

Used to re-

fine this method for subsequent events.
The method of elliptical approximations drew ellipses over [the hodograph between wind levels.

The minor axes of the ellipses werq determined

by the amount of change in wind direction between wind layers.

The radia-

tion intensity associated with the ellipses was based on scali

and past

experience.

the Ne-

The method was based largely on empirical data fr

vada Proving Ground (NPG), and it had been used successfully td

predict

the fallout fields from low-yield PPG detonations.
As the tests began, it became apparent that a more accurat

method was

The la

e differ-

ences between NPG and PPG shot yields and cloud heights made t

accuracy

needed to clearly define the fallout from high yields.

of using elliptical approximations for CASTLE shots suspect.

ere was no

assurance that the high-yield fallout mechanisms were described

at all.

For example, the trapping characteristics of the atmospheric

ndary with

the stratosphere

(the tropopause) could only be conjectured, a

even if

* Because little was known about the fallout mechanism of high-pield events
and because of errors in other parameters of the fallout fore
additional safety factor was assumed necessary, even though t

the factor could not be precisely stated. For CASTLE, the es
the diffusion-caused widening of the fallout-contaminated are

with dis-

tance was increased by the addition of a 15° sector on each s de of the

calculated fallout area.
{Reference 16, p. 61).

In previous operations the factor u ed was 10°

lil

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