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PNNL-13501 - Pacific Northwest National Laboratory

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Study Control Number: PN00078/1485<br />

Reactor Transmutation of Waste<br />

Rick J. Migilore<br />

Technetium-99 and iodine-129 are long-lived fission products generated during the normal operation of a nuclear reactor.<br />

Methods were studied on ways to transmute these radionuclides into nonhazardous forms and thereby eliminate the longterm<br />

risks associated with their disposal in a repository.<br />

Project Description<br />

The purpose of this project is to determine the amounts of<br />

technetium-99 (Tc-99) and iodine-129 (I-129) that may be<br />

transmuted into stable isotopes using existing commercial<br />

nuclear reactors. It would be advantageous to destroy<br />

these long-lived isotopes, and to mitigate the associated<br />

long-term risks of storing and containing them in the<br />

Yucca Mountain repository. The computer program<br />

Monte Carlo N-Particle (MCNP) transport code was used<br />

for the transmutation calculations. We estimated that<br />

approximately 63% of the projected Tc-99 inventory and<br />

35% of the projected I-129 inventory could be transmuted<br />

during the years 2010 through 2030 using existing light<br />

water reactors. This concept appears to be feasible, as<br />

commercial nuclear reactors can be designed to burn more<br />

of these isotopes than they produce.<br />

Introduction<br />

Reactor transmutation of waste has been studied<br />

extensively over the past 25 years using a variety of<br />

calculational methods and reactor types (Wachter and<br />

Croff 1980; Binney et al. 1990; Wootan et al. 1992;<br />

Abrahams et al. 1995). The goal of waste transmutation<br />

studies is to demonstrate that reactor waste can be<br />

destroyed, thereby circumventing the risks associated<br />

with disposing of the waste in an underground repository.<br />

The spent fuel repository slated to be built at Yucca<br />

Mountain must comply with federal regulations for a<br />

period of 10,000 years, although the risks to the public do<br />

not end after that time. Reactor transmutation of waste<br />

would eliminate the long-lived fission products in the<br />

waste stream, leaving only shorter-lived fission products<br />

to be disposed. Reactor transmutation of waste would<br />

reduce the required repository confinement lifespan to<br />

500 years or less, because after that time the waste would<br />

be no more radioactive than the original uranium ore.<br />

Most transmutation studies include transmutation of<br />

actinides (heavy metals such as plutonium, neptunium,<br />

etc.) in addition to transmutation of fission products such<br />

as Tc-99 and I-129. The current study focused only on<br />

the transmutation of long half-life fission products Tc-99<br />

and I-129 and assumed that all actinides are recycled.<br />

Tc-99 and I-129 are transmuted to stable isotopes by the<br />

following reactions:<br />

99 Tc + n ➝ 100 Tc ➝ 100 Ru (stable) 16s (β - )<br />

129I + n ➝ 130 I ➝ 130 Xe (stable) 12.4h (β - )<br />

Further irradiation of Ru-100 and Xe-130 leads only to<br />

stable isotopes. Xenon-130 is a gas and that the target<br />

must be designed to accommodate the increase in pressure<br />

from buildup of radioxenon.<br />

Tc-99 is metallic and may be formed into slugs for<br />

irradiation without difficulty. I-129, conversely, is a gas<br />

and must be bonded with another material prior to<br />

irradiation. For the purposes of this study, solid<br />

vanadium iodide (VI2) was selected as the form to be<br />

irradiated. Vanadium iodide was selected for both its<br />

high density (5.44 g/cm 3 ) and high melting temperature<br />

(1431°F). The stability of this compound in a true<br />

radiation environment is unknown. Iodine compounds<br />

may be corrosive to cladding materials.<br />

Approach<br />

The MCNP reactor physics code was used to calculate the<br />

instantaneous transmutation rate for each of the nuclides.<br />

A simplified 3000 MWt pressurized water reactor core<br />

was modeled using 17x17 fuel assemblies. Each fuel<br />

assembly has 24 locations that may be used for inserting<br />

fission product target rods. To maximize the quantity of<br />

fission product targets that may be inserted into the<br />

reactor, all of the target locations are filled with target<br />

rods. In reality, this would not be possible, as locations<br />

must be retained for control rods. Six different cases<br />

were executed.<br />

Nuclear Science and Engineering 369

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