The depth distribution of fallout depends greatly upon the
thermocline, which is the layer of water between the warmer, surface
zone and the colder, deepewater zone in a thermally stratified body
of water.

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The termocline is consequently a loyer with a large temperaf

ture acadient with depth.

In the area ofEniwetok Atoll, the surface

layer is less than 100 meters thick.

Because the temperature is

fairly uniform throughout this upper layer, mixing in this layer
requires only small amounts of energy and should occur easily.

In

contrast, transfer of materials across the thermocline layer by turbui

lent diffusion is much slower since the thermocline is a layer of high

stability.

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In studies during the 1958 test series at Eniwetok Atoll, analyses
trrara moda hy filtratian ta dictinenich hetween particulate matter and
colloidal-soluble matter.

The particulate fraction was considered in

these studies to be greater than 0.45 microns and the colloid-solubie
fraction was considered to be smaller.

At 48 hours after the nuclear

explosion, the major part of the total radioactivity was concentrated
at the 100-meter depth of the upper edge of the thermocline.

Logically,

the particulate matter would be expected to sink much more rapidly.
This was confirmed by observations up to six-weeks later, all of which
showed that the colloid-soluble fraction was always on order of
magnitude greater in the surface zone than the particulate fraction.

At the 400-meter greatest depth observed, the particulate fraction
increased in time from beingan order of magnitude less until it
approached the colloid-soluble fraction in magnitude at the end of

this six-weeks period.
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