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Management of Commercially Generated Radioactive Waste - U.S. ...

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5.74<br />

Fuel Reprocessing <strong>Waste</strong><br />

Spent Fuel HLW RH & CH-TRU<br />

Salt 51,000 MTHM(a) 62,000 MTHM 100,000 MTHM<br />

Granite 122,000 69,000 108,000<br />

Shale 64,000 30,000 56,000<br />

Basalt 122,000 56,000 92,000<br />

If the amount <strong>of</strong> disposed waste, rather than the size <strong>of</strong> the repository, were held constant,<br />

the radiological consequences would be the same for each geologic medium. In other words,<br />

once the radionuclides are outside the repository proper, their movement away from the<br />

repository is governed by the same set <strong>of</strong> assumptions regardless <strong>of</strong> repository media. (This<br />

limitation <strong>of</strong> the analysis would be improved upon in site-specific analyses when site spe-<br />

cific data or sorptive properties <strong>of</strong> adjacent rock become available.)<br />

In the case <strong>of</strong> faulting and flooding with stream transport the assumption was made that<br />

the same amount <strong>of</strong> waste was removed by water regardless <strong>of</strong> repository medium. Repository<br />

medium affected consequences only in salt repositories; the presence <strong>of</strong> salt along with the<br />

wastes would likely preclude use <strong>of</strong> the emergent stream as a source <strong>of</strong> drinking water or<br />

food. Thus, except for the case <strong>of</strong> salt entering the biosphere with the waste radionuc-<br />

lides, no analysis was made <strong>of</strong> the waste repository medium's influence in the consequences<br />

<strong>of</strong> the postulated long-term events.<br />

In the case <strong>of</strong> human intrusion by drilling, the same amount <strong>of</strong> waste was assumed to be<br />

brought to the surface regardless <strong>of</strong> repository media.<br />

5.5.1 Repository Breach by Meteorite<br />

Breach <strong>of</strong> a repository would be possible by a meteorite estimated to be about 25 m in<br />

diameter striking a point on the surface above the center <strong>of</strong> the repository at a speed <strong>of</strong><br />

about 20 km/sec on impact. If the meteorite's density is 8 g/cm 3 (which is representative<br />

<strong>of</strong> iron or nickel-iron meteorites), the mass <strong>of</strong> the meteorite at contact would be about 6.5<br />

x 104 MT and would have an energy equivalent to about 3 megatons <strong>of</strong> TNT. This meteorite<br />

would produce a crater roughly 2 km in diameter at the surface and 600 m deep at its deepest<br />

point. No clear evidence is available to suggest that meteorites <strong>of</strong> this size have created<br />

craters this deep over the age <strong>of</strong> the earth. On the other hand, the presence <strong>of</strong> astroblemes<br />

suggests that the earth has been hit by very large extraterrestrial bodies (Claiborne and<br />

Gera, 1978).<br />

Temperatures at the impact point <strong>of</strong> the meteorite strike would reach millions <strong>of</strong><br />

degrees, and most <strong>of</strong> the meteorite plus some <strong>of</strong> the surrounding rock would be vaporized.<br />

Some <strong>of</strong> the rock material would be pulverized and ejected into the air as the crater formed.<br />

Most <strong>of</strong> the ejected material would fall back into the crater and its immediate vicinity.<br />

(a) Metric tons <strong>of</strong> heavy metal in the case <strong>of</strong> spent fuel or spent fuel equivalent in the<br />

case <strong>of</strong> reprocessing wastes.

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