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Going Nuclear: Notes from the officially unofficial book tour
I work in the analytical labs at one of Europe’s oldest and largest nuclear sites: Sellafield, in northwestern England. I spend my days at the fume hood front, pipette in one hand and radiation probe in the other (and dosimeter pinned to my chest, of course). Outside the lab, I have a second job: I moonlight as a writer and public speaker. My new popular science book—Going Nuclear: How the Atom Will Save the World—came out last summer, and it feels like my life has been running at full power ever since.
P. J. Maudlin, K. O. Ott, R. C. Borg
Nuclear Science and Engineering | Volume 72 | Number 2 | November 1979 | Pages 140-151
Technical Paper | doi.org/10.13182/NSE79-A19459
Articles are hosted by Taylor and Francis Online.
Breeding estimates for long-term reactor fuel logistics are pursued, specifically deriving an instantaneous or transitory fuel growth rate definition, γ(t), from the basic space- and time-dependent fuel cycle equations. The derivation is valid for either the discontinuous or continuous fuel cycle treatments. The resulting definition is applied to a uranium-plutonium fast reactor operating in the closed fuel cycle mode. Transitory growth rate results are calculated for various fuel isotopic weight-factor sets and initial fuel compositions. These results show γ(t) to be practically independent of the isotopic weight-factor sets, provided the γ(t) is calculated from the time-dependent variation of the fuel isotopes. The growth rate derivation automatically yields the fuel composition shift in the form of the reactor fuel time derivative. Investigations of the impact of this quantity on transitory breeding descriptions show that it is the erroneous neglect of the fuel composition-shift term that induces the previously observed strong dependence of the growth rate upon the fuel isotopic weight-factor sets. Accurate approximation of the instantaneous fuel growth rate using transitory static reaction rate information (fuel-shift term neglected) is shown possible with the substitutional critical mass (CM) worth weights, .