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The FuTure oF nuclear Fuel cycle - MIT Energy Initiative

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[http://nextgeneration<strong>nuclear</strong>plant.com/index.shtml] by the U.S. Department of <strong>Energy</strong><br />

uses helium coolant. <strong>The</strong> technology for gas-cooled reactors is available today at temperatures<br />

up to ~850°C. Recently there has been work on using low-pressure liquid salts as coolants—the<br />

Advanced High-Temperature Reactor. Recent studies of the liquid-salt cooled<br />

AHTR (Appendix B) indicate the potential for lower costs (Peterson, Griveau), but the<br />

technology is not as fully developed. Most HTR R&D supports the use of either coolant.<br />

<strong>The</strong> coated-particle fuel has four potential unique characteristics that may provide major<br />

societal benefits and thus the incentives for the federal government to encourage the development<br />

of such a reactor. <strong>The</strong>se benefits have not been fully quantified or proven.<br />

Safety<br />

<strong>The</strong> high-temperature capability of the fuel enables a different approach to reactor safety<br />

that may offer major benefits. In traditional LWRs, if a large reactor is shut down and cooling<br />

to the reactor core stops, the reactor core will heat up and melt. This is what occurred<br />

during the Three Mile Island accident. HTRs can be designed such that if the reactor cooling<br />

fails, the heat can be transferred by conduction and convection processes to the environment.<br />

This is possible because (1) the fuel can go to very high temperatures without failing<br />

and provide a very large temperature drop to enable heat transport to the environment<br />

and (2) the low power density [dilute fuel] that results in the very slow heatup of the reactor<br />

core after shutdown. In effect, many safety functions are transferred from the reactor<br />

(emergency safety systems) and the reactor operator to the fuel fabricator who is required<br />

to make a fuel that can withstand extreme conditions.<br />

Safeguards and Nonproliferation<br />

<strong>The</strong> two nonproliferation concerns associated with the <strong>nuclear</strong> fuel <strong>cycle</strong> are: (1) uranium<br />

enrichment on the front end that could provide a route to producing weapons-useable<br />

high-enriched uranium and (2) plutonium separation from SNF on the back end. HTRs<br />

require low-enriched uranium and thus have most of the same front-end concerns as associated<br />

with LWRs. However, HTR SNF is different from SNF of other types of power<br />

reactors. <strong>The</strong> plutonium content of HTR SNF from currently proposed reactors would be<br />

so low as to approach the International Atomic <strong>Energy</strong> Agency limits for the termination of<br />

safeguards; that is, the difficulty of fissile material recovery is so great that anyone wanting<br />

to obtain weapons-useable materials would likely choose an alternative route to obtain such<br />

materials (Durst 2009). <strong>The</strong>re are several reasons for this (Moses, 2010).<br />

p Burnup. HTR SNF burnup is typically 50% higher than LWR SNF resulting in less attractive<br />

plutonium isotopic mix for weapons.<br />

p Plutonium content. <strong>The</strong> SNF plutonium concentration is low (~570 ppm for some designs)<br />

and because the fissile plutonium is diluted with carbon, silicon carbide, and<br />

graphite. One must divert almost 20 m 3 of SNF to have a significant quantity of plutonium—the<br />

quantity of concern in terms of building a <strong>nuclear</strong> weapon.<br />

p Chemical form. <strong>The</strong> technical and economic difficulties in recovering fissile materials<br />

from HTR SNF are significantly greater than for other types of SNF because (1) the fissile<br />

210 <strong>MIT</strong> STudy on <strong>The</strong> <strong>FuTure</strong> <strong>oF</strong> <strong>nuclear</strong> <strong>Fuel</strong> <strong>cycle</strong>

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