Quantities of '''C that may be formed in the fuel and core structural materials of light-water-cooled reactors (LWRs), in high-temperature gas-cooled reactors (HTGRs), and in liquid-metal-cooled fast breeder reactors (LMFBRs) have been calculated by use of the ORIGEN code.' Information supplied by five LWR-fuel manufacturers pertaining to nitride nitrogen and gaseous nitrogen in their fuels and fuel-rod void spaces was used in these calculations. Average nitride nitrogen values range from 3 to 50 ppm (by weight) in LWR fuels, whereas gaseous nitrogen in one case is equivalent to an additional 10 to 16 ppm. Nitride nitrogen concentrations in fast-flux test facility (FFTF) fuels are 10 to 20 ppm. The principal reactions that produce '''C involve '''N, ' O, and (in the HTGR) "C. Reference reactor burnups are 27,500 MWd per metric ton of uranium (MTU) for boiling water reactors (BWRs), 33,000 MWd for pressurized water reactors (PWRs), about 95,000 MWd per metric ton of heavy metal (MTHM) for HTGRs, and 24,800 MWd/ MTHM for an LMFBR with nuclear parameters that pertain to the Clinch River Breeder Reactor. Nitride nitrogen, at a median concentration of 25 ppm, contributes 14, 15, and 6 Ci of "C/GW(e)-yr to BWR, PWR, and LMFBR fuels, respectively. The contribution of "O in BWR and PWR fuels is 3.3 and 3.5 Ci of "C/GW(e)-yr, respectively, but it is less than 0.2 Ci/GW(e)-yr, in blended LMFBR fuel. In the HTGR fuel particles (UCj or ThO;), 10 Ci of "C/GW(e)-yr will be formed from 25 ppm of nitrogen, whereas "O in the ThO: will contribute an additional 2 Ci/GW(e)-yr. All '^C contained in the fuels may be released in a gas mixture (CO2, CO, CH4, etc.) during fuel dissolution at the fuel reprocessing plants. However, some small fraction may remain in aqueous raffinates and will not be released until these are converted to solids. The gases would be released from the plant unless special equipment is installed to retain the '''C-bearing gases.Cladding metals and other core hardware will contain significant quantities of '^C. Very little of this will be released from BWR, PWR, and LMFBR hardware at fuel reprocessing plants; instead, the contained '""C, 30 to 60 Ci/GW(e)-yr for LWRs and about 13 Ci/GW(e)-yr for a CRBR, will remain within the metal, which will be retained on site or in a Federal repository. The only core structural material of HTGRs will be graphite, which will contain 37 to 190 Ci of '''C/GW(e)-yr, exclusive of that in the fuel particles, if the graphite (fuel block and reflector block) initially contains 0 to 30 ppm of nitrogen. All of this is available for release at a fuel reprocessing plant if the graphite is burned to release the fuel particles for further processing. Special equipment could be installed to retain the ''C-bearing gases.
During the two years prior to his death in Xanuary lS7/y R. B. Evans ITI had performed many experiments onT the dixf;v?"x'm o'£ cesium in various types of graphite. A. L-Sutton, Jr., ant: S. L. "/oNns were collaborators in some of this work, which was a.continuation of-that summarized on pp. 154-81 in High Tenper&'Zuf'£ Gees-Socle* Suitor Base-Technology Vrog-'frn Progress Report* Jcznuaru I, 1974-Ji^x ZO, 1975 (ORNL-5108). In this report, Evans and Saccoh presented a rtfery iuvmlving diffusiotnal transport and first-order irreversible reaction of cesit^c in graphite. However, only a few experiments were available; re test th* 1 theory. ''''-; ; At the time of his death, Evans had outlined f r written about bslt of a report on the cesium-diffusion experiments. That material did not include a presentation or an analysis of tfc« data, c tatk which he had apparently only just started. His writings did include a more delailea presentation of theory. During the past year and a half, we have extracted the experimental data on cesium diffusion in graphite from various notebooks and ha/e com pleted and corrected those sections of the report that Evans had started to write or had already written. This report presents, these two items. I 37 It also presents an analysis of data on diffusion of ' Ci; in Hawfcer-Siddeley graphite but does not contain an analysis of the data on other graphites in terms of theory presented by £v3ns and Sutton. As the reader will note in the Appendix A, there ar« many experimental results, the analyses of which should add greatly to our knowledge of the procesaeg that control the transport of cesium in at i*>ast five types of graphites, We are not presently performing analyses cf these data; is: is, however, part of the purpose of this report to ma!;a tU? data available to other workers so that they may be able to test rh«;ir own theories.
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