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Salt Disposal of Heat-Generating Nuclear Waste

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and DHLW over-test were designed to identify how the host rock and the disposal<br />

room respond to the excavation itself and then to the heat generated from waste<br />

placed in vertical holes in the drift floor. These tests imparted a relatively modest<br />

thermal load in a vertical borehole arrangement and did not use crushed-salt<br />

backfill or explore reconsolidation <strong>of</strong> salt. They primarily focused on the<br />

mechanical response <strong>of</strong> the salt under modest heat load. The results can be used,<br />

for example, to validate the next-generation high-performance codes over a<br />

portion <strong>of</strong> the multiphysics functionalities. The <strong>Heat</strong>ed Axisymmetric Pillar test<br />

involved an isolated, cylindrically shaped salt pillar and provides an excellent<br />

opportunity to calibrate scale effects from the laboratory to the field, as well as a<br />

convenient configuration for computer model validation (Matalucci 1987).<br />

1985–1990. A set <strong>of</strong> moisture transport and release tests were part <strong>of</strong> the<br />

borehole plugging and sealing test series at WIPP and were designed to measure<br />

moisture release associated with heated boreholes and to evaluate transport<br />

mechanisms. Each borehole contained a nitrogen flow and a water vapor<br />

collection and measurement system. Water vapor flowing in the nitrogen was<br />

collected and weighed (Nowak and McTigue 1987). These data characterizing<br />

brine movement and accumulation were interpreted in terms <strong>of</strong> a model for flow<br />

in a saturated porous medium. Comparisons between model calculations and brine<br />

inflow rates showed order-<strong>of</strong>-magnitude agreement for permeability in accord<br />

with independent in situ determinations <strong>of</strong> permeability in the salt. Expected<br />

accumulations <strong>of</strong> brine in typical WIPP waste disposal rooms were calculated by<br />

numerical methods using a mathematical description for the brine inflow model.<br />

Brine accumulation in a disposal room was calculated to be in the range <strong>of</strong> 4 m 3 to<br />

43 m 3 in 100 years. The maximum expected accumulation, 43 m 3 , is 1.2% <strong>of</strong> the<br />

initial room volume, about the same as the quantity <strong>of</strong> brine in the salt that was<br />

removed by mining the room (Nowak, McTigue, and Beraun 1988).<br />

1986–1991. An in situ test <strong>of</strong> simulated HLW glass and other waste package<br />

components was conducted at WIPP beginning in 1986 in a program known as<br />

the Materials Interface Interactions Test (MIIT). The MIIT involved<br />

approximately 1,900 samples in 50 test boreholes, with specimens that included<br />

16 variations <strong>of</strong> simulated HLW glass, 11 potential canister metals, rock salt, and<br />

two brine solutions (Wicks and Molecke 1988). The MIIT included a 5-year study<br />

<strong>of</strong> the burial <strong>of</strong> simulated waste glasses and the resulting long-term waste-glass<br />

leaching behavior. Brine analyses were performed on samples from selected<br />

boreholes containing simulated waste-glass specimens, resulting in release rates<br />

<strong>of</strong> less than one part in 100,000 for all elements investigated (Wicks 2001).<br />

1.4 Analogues for <strong>Salt</strong> <strong>Disposal</strong><br />

As this report acknowledges, some key issues pertaining to HLW disposal in salt<br />

need attention if a salt disposal option is selected. These remaining issues should<br />

not be misconstrued to imply the scientific basis for salt disposal is weak. It is<br />

not. <strong>Salt</strong> disposal remains a very favorable option for the U.S. The most likely<br />

future for HLW salt disposal includes permanent, dry encapsulation.<br />

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