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DOE, General Matter team up for new fuel mission at Hanford
The Department of Energy's Office of Environmental Management (EM) on Tuesday announced a partnership with California-based nuclear fuel company General Matter for the potential use of the long-idle Fuels and Materials Examination Facility (FMEF) at the Hanford Site in Washington state.
According to the announcement, the DOE and General Matter have signed a lease to explore the FMEF's potential to be used for advanced nuclear fuel cycle technologies and materials, in part to help satisfy the predicted future requirements of artificial intelligence.
Jakob Weitman
Nuclear Science and Engineering | Volume 18 | Number 2 | February 1964 | Pages 246-259
Technical Paper | doi.org/10.13182/NSE64-A18325
Articles are hosted by Taylor and Francis Online.
The effective resonance integral of thorium oxide rods has been determined as a function of their surface-to-mass ratio. The range of S/M values covered is 0.15 - 0.65 cm2/g. An experimental technique based on the comparison of activities obtained in thermal and slowing-down neutron fluxes was employed. The shape of the resonance neutron spectrum was determined from measurements with a fast chopper and from calculations, permitting deduction of a correction factor which relates the experimental values to the ideal 1/E case. The results are summarized by the following expression: The main contribution to the margin of error arises from the uncertainties in the 4% spectral correction applied, in the 1.5 b “l/v” part deducted and in the 1510 b infinite-dilution integral of gold, used as a standard. In order to compare the consistency of Dresner's first equivalence theorem and Nordheim's numerical calculations relative to our results, the resonance integral values for thorium metal rods obtained previously by Hellstrand and Weitman have been recalculated, using recent cross section and spectrum data. The new formula is It differs from the old one mainly because of the proved non-l/v behaviour of the thorium cross section below the first resonance.