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

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K.8<br />

In the very-near-field analyses, the baseline canister-emplacement design was a single<br />

overpacked canister placed in a hole. In general, the void space between the sleeve and<br />

the hole was assumed to be backfilled with crushed rock. In each <strong>of</strong> the HLW calculations,<br />

a 15-cm annulus <strong>of</strong> crushed or fractured rock was assumed.<br />

K.1.2 Thermal Loadings Achieved in Conceptual Repository Designs<br />

Engineering or operational constraints may restrict any <strong>of</strong> the thermal loadings dis-<br />

cussed in the above section to values lower than the limits presented in Table K.1.2. These<br />

constraints include such factors as reasonable HLW concentration in canisters, available<br />

canister sizes, permissible hole spacing, and room stability limitations on hole arrange-<br />

ments. Spent-fuel canister loading is limited in this Statement to a single PWR or BWR<br />

spent fuel assembly so that canister heat loads are below limiting values. The HLW canister<br />

diameters are reduced as necessary in each case so that the canister loadings are below the<br />

limits <strong>of</strong> Table K.1.2. Alternatively the waste could be diluted with inert material without<br />

reducing canister sizes to achieve the same result.<br />

As a hedge against uncertainties in the criteria and other factors and to ensure a con-<br />

servative estimate <strong>of</strong> repository capacities, the design areal thermal lodaings for both<br />

spent fuel and HLW were established at 2/3 <strong>of</strong> this limiting areal loading parameter in<br />

Table K.1.2. The age <strong>of</strong> both the spent fuel and HLW were assumed to be 6.5 years. Using<br />

the criteria in Table K.1.2 for 6.5-year-old waste provided a further degree <strong>of</strong> conservatism<br />

since the criteria were developed for 10-year-old waste (the thermal limits could be<br />

increased for younger wastes). The resulting thermal densities actually achieved in the<br />

first conceptual repositories are listed in Table K.1.4. The limiting thermal parameter,<br />

i.e., near-field or far-field, is denoted by an asterisk. In the case <strong>of</strong> BWR fuel in shale<br />

and the RH-TRU waste in all media except salt, structural limitations on canister place-<br />

ments limit thermal loading.<br />

Temperature pr<strong>of</strong>iles calculated for the conceptual repositories using the achieved<br />

loadings are shown in Figures K.1.1 through K.1.8. The pr<strong>of</strong>iles show temperature increases<br />

above ambient temperature as a function <strong>of</strong> depth at several times after the repository is<br />

loaded, for both spent fuel and HLW and for the four geologic media. For example, the pro-<br />

files for a spent fuel repository at a depth <strong>of</strong> 600 m in salt with the average loadings <strong>of</strong><br />

Table K.1.4, are shown in Figure K.I.1. The figure shows that the temperature at the repos-<br />

itory depth reaches a maximum value about 70 years after emplacement. The calculation is<br />

made assuming that the heat source is uniformly dispersed at the repository level. The tem-<br />

perature is calculated along a line perpendicular to the plane <strong>of</strong> the repository and passing<br />

through the center <strong>of</strong> the emplacement area. Actual temperatures in the vicinity <strong>of</strong> the<br />

repository level will vary with the discontinuities <strong>of</strong> the temperature pr<strong>of</strong>ile around each<br />

canister.<br />

Figure K.1.2 gives the pr<strong>of</strong>iles for the repository in salt for the high-level waste<br />

from the reprocessing cycle. Corresponding pr<strong>of</strong>iles for each cycle are shown in Fig-<br />

ures K.1.3 and K.1.4 for granite, K.1.5 and K.1.6 for shale, and K.1.7 and K.1.8 for basalt<br />

repositories.

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