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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 />

atoms by tritium can also occur for tritium <strong>of</strong> anthropogenic orig<strong>in</strong>, as well as for molecules<br />

o<strong>the</strong>r than water that conta<strong>in</strong> hydrogen atoms. For example, at room temperature, <strong>the</strong><br />

comb<strong>in</strong>ation <strong>of</strong> hydrogen gas (H2) and T2 to produce HT is favoured (Jones, 1948).<br />

Isotopes <strong>of</strong> <strong>the</strong> same element take part <strong>in</strong> <strong>the</strong> same chemical reactions, but because <strong>the</strong> atoms<br />

<strong>of</strong> different isotopes differ <strong>in</strong> terms <strong>of</strong> <strong>the</strong>ir size and atomic weight, <strong>the</strong>y tend to react at<br />

different rates. For example, physical processes, such as evaporation and diffusion, can<br />

discrim<strong>in</strong>ate aga<strong>in</strong>st heavy isotopes because <strong>the</strong>y move more slowly <strong>in</strong> <strong>the</strong> environment.<br />

In addition, enzymatic discrim<strong>in</strong>ation and differences <strong>in</strong> k<strong>in</strong>etic characteristics and equilibria<br />

can result <strong>in</strong> reaction products that are isotopically heavier or lighter than <strong>the</strong>ir precursor<br />

materials. In <strong>the</strong> case <strong>of</strong> hydrogen isotopes, although tritium closely follows <strong>the</strong> reactions<br />

<strong>of</strong> ord<strong>in</strong>ary hydrogen, <strong>the</strong> relatively large mass differences between <strong>the</strong> hydrogen isotopes<br />

(as shown <strong>in</strong> Table 3.1) make isotopic effects easily discernible (Jacobs, 1968).<br />

Table 3.1: Atomic Weights <strong>of</strong> Different Hydrogen Isotopes Contribut<strong>in</strong>g to Isotopic<br />

Fractionation <strong>in</strong> <strong>the</strong> Environment (from Lange and Forker, 1961).<br />

Hydrogen Isotope Symbol Atomic Weight (g)<br />

Proton 1 H 1.00814 ± 0.000003<br />

Deuteron 2 H 2.014735 ± 0.000006<br />

Triton 3 H 3.016997 ± 0.000011<br />

As discussed above, physical processes, such as phase changes, that can <strong>in</strong>fluence tritium<br />

transport <strong>in</strong> <strong>the</strong> environment are expected to be slower for heavier isotopes. For example,<br />

Table 3.2 provides a summary <strong>of</strong> some key <strong>the</strong>rmodynamic properties for <strong>the</strong> different<br />

oxides <strong>of</strong> hydrogen isotopes, <strong>in</strong>clud<strong>in</strong>g H2O, D2O and T2O (Bigeleisen, 1962; Jacobs,<br />

1968; Smith and Fitch, 1963). Based on <strong>the</strong>se data, <strong>in</strong>creases <strong>in</strong> boil<strong>in</strong>g po<strong>in</strong>t and heat<br />

<strong>of</strong> vaporization can be discerned with <strong>in</strong>creas<strong>in</strong>g atomic weight <strong>of</strong> <strong>the</strong> hydrogen isotopes.<br />

Such physical differences between hydrogen isotopes would be expected to lead to<br />

correspond<strong>in</strong>g decl<strong>in</strong>es <strong>in</strong> <strong>the</strong> rates <strong>of</strong> evaporation <strong>in</strong> nature for isotopically heavier water<br />

molecules that have relatively higher boil<strong>in</strong>g po<strong>in</strong>ts and heats <strong>of</strong> vaporization. In addition,<br />

isotopes with higher entropies could lead to <strong>in</strong>creased rates <strong>of</strong> mix<strong>in</strong>g.<br />

Table 3.2: Thermodynamic Properties <strong>of</strong> <strong>the</strong> Oxides <strong>of</strong> Hydrogen Isotopes<br />

(Bigeleisen, 1962; Jacobs, 1968; Smith and Fitch, 1963).<br />

Oxide <strong>of</strong> Hydrogen Isotope<br />

Thermodynamic Property H2O D2O T2O<br />

Boil<strong>in</strong>g po<strong>in</strong>t ( o C) 100.00 101.42 101.51<br />

Triple-po<strong>in</strong>t temperature ( o C) 0.010 3.82 4.49<br />

Triple-po<strong>in</strong>t pressure (mmHg) 4.58 5.02 4.87<br />

Heat <strong>of</strong> vaporization at <strong>the</strong><br />

boil<strong>in</strong>g po<strong>in</strong>t (kcal/mole) 9.72 9.9 10.1<br />

Entropy (at 298 K) 16.75 18.9 19.0<br />

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