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_ September

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YARTIN : RADIOECOLOGY AND STUDY OF ENVIRONMENTAL RADIATION

297

in the mid-latitudes of the northern hemisphere is higher in late winter and
early spring than at any other time of year (Fig. 4).
Several hypotheses have been offered to explain these latitudinal and
seasonal variations in the amounts and rate of stratospheric fallout but several important issues have not yet been resolved (Arnold and Martell 1959,

Libby 1956a, 1956b, 1957, 1958, 1959, Machta 1959, Machta and List 1956a,
1956b, 1958, Martell and Drevinsky 1960, and Stewart et al. 1957).
Estimates of the residence time or effective half-life of radioactive debris

in the stratosphere have ranged from ‘‘a matter of months’’ (Martell and
Drevinsky 1960) to as much as 5 to 10 years (Libby 1956a). Apparently, the
residence time and rate of stratospheric fallout are not uniform but tend to
decrease with decreasing altitude and with increasing latitude of introduction. The rate of stratospheric fallout is highest for materials introduced in

the lowest part of the stratosphere at high latitudes and lowest for materials

introduced at higher altitudes near the equator.
In both the troposphere and the stratosphere the transport of materials
is toward the northeast at mid-latitudes and toward the southwest at higher
latitudes. In mid-latitudes, the transfer of the stratospheric materials into
the troposphere probably occurs in the vicinity of the subtropical jet stream.

At high latitudes, this transfer occurs in high pressure (anti-cyclone) areas

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where there is a pronounced subsidence of stratospheric air during late
winter and early spring. In both hemispheres the rate at which stratospheric
materials are removed from the troposphereis closely related to precipitation
patterns. The inter-hemispheric exchange of atmospheric debris probably
occurs in conjunction with the seasonal, latitudinal migration of global high
and low pressure belts and their associated wind systems.
The actual processes involved in these exchanges between the stratosphere
and troposphere and between the northern and southern hemispheres are

imperfectly understood. Studies now in progress may help to resolve a variety of questions concerning the mechanismsof stratospheric and tropospheric

fallout, but the solution of these problems will probably be a greater boon
to meteorology than to radioecology.
The critical problems in radioecology are related to the measurable aspeets of fallout rate and the distribution of particular radionuclides. The
radionuclides generally considered to be most important in the evaluation of
the potential biclogical hazards of world-wide fallout are C-14, Sr-90 and Cs187. The C-14 produced by nuclear detonations and suspended in the atmosphere as C“O, mayeventually be distributed uniformly in the atmosphere
of both hemispheres. Most of the Sr-90 and Cs-137 will probably be deposited
in the northern hemisphere between 30° and 60° latitude.
A better understanding of the mechanisms which determine the rate and
geographical distribution of world-wide fallout would be of particular value

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