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Investigation of the Environmental Fate of Tritium in the Atmosphere

Investigation of the Environmental Fate of Tritium in the Atmosphere

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INVESTIGATION OF THE ENVIRONMENTAL FATE OF TRITIUM IN THE ATMOSPHERE<br />

contribution <strong>of</strong> HT to total tritium levels (Harteck, 1954). The tritium concentration <strong>in</strong><br />

atmospheric hydrogen is expected to rema<strong>in</strong> relatively stable, whereas localized variability<br />

<strong>in</strong> ra<strong>in</strong>water tritium levels may occur (Harteck, 1954; Libby, 1953).<br />

In <strong>the</strong>rmonuclear clouds, tritiated hydrogen is produced <strong>in</strong> <strong>the</strong> stratosphere by radiative<br />

dissociation <strong>of</strong> water under oxidiz<strong>in</strong>g conditions (Martell, 1963). Tritiated methane is formed<br />

through tropospheric exchange <strong>of</strong> methane with <strong>the</strong> tritiated hydrogen that has moved down<br />

from <strong>the</strong> stratosphere. The tritium specific activity <strong>of</strong> atmospheric methane is several orders<br />

<strong>of</strong> magnitude higher than that <strong>of</strong> ra<strong>in</strong>fall, but somewhat less than that <strong>of</strong> atmospheric<br />

hydrogen and stratospheric water vapour (Harteck, 1954).<br />

Follow<strong>in</strong>g production <strong>in</strong> <strong>the</strong> upper atmosphere by cosmic radiation, tritium atoms have a high<br />

k<strong>in</strong>etic energy and are readily oxidized (Jacobs, 1968). At lower than atmospheric pressures,<br />

this likely predom<strong>in</strong>antly occurs through a three-body collision with oxygen (O2) to <strong>in</strong>itially<br />

form a relatively stable radical, HO2 (Harbeck, 1954). This radical can <strong>the</strong>n react with ozone<br />

(O3) follow<strong>in</strong>g repeated photochemical decomposition reactions <strong>of</strong> TO2 to form HTO, as<br />

opposed to HT, <strong>in</strong> <strong>the</strong> atmosphere. Once tritium has been <strong>in</strong>corporated <strong>in</strong>to water molecules,<br />

HTO <strong>the</strong>n falls to <strong>the</strong> surface <strong>of</strong> <strong>the</strong> earth as ra<strong>in</strong> and snow, enter<strong>in</strong>g <strong>the</strong> natural hydrological<br />

cycle <strong>in</strong> this way (Figure 3.1; Stamoulis et al., 2005; UN, ILO and WHO, 1983).<br />

A second feasible <strong>in</strong>itial reaction would <strong>in</strong>volve <strong>the</strong> collision <strong>of</strong> tritium with an H2 molecule,<br />

with a resultant isotopic exchange to form HT. Small amounts <strong>of</strong> tritium, represent<strong>in</strong>g less<br />

than 1% <strong>of</strong> <strong>the</strong> amount produced per day, may also be produced through <strong>the</strong> <strong>in</strong>itiation <strong>of</strong> a<br />

reaction between tritium and oxygen by <strong>the</strong> beta radiation from tritium decay (Dorfman and<br />

Hemmer, 1954; Yang and Gevantman, 1960).<br />

Transfer <strong>of</strong> tritiated water vapour from <strong>the</strong> stratosphere to <strong>the</strong> troposphere occurs with a halftime<br />

<strong>of</strong> approximately a year, after which it is deposited onto <strong>the</strong> earth’s surface as ra<strong>in</strong>fall<br />

and through molecular exchange with a half-time on <strong>the</strong> order <strong>of</strong> 10 days. Deposited HTO<br />

is <strong>the</strong>n transported <strong>in</strong> <strong>the</strong> environment as part <strong>of</strong> <strong>the</strong> hydrological cycle (Figure 3.1; Jacobs,<br />

1968).<br />

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