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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.
Steve Kahn, Randall Harman, Vernon Forgue
Nuclear Science and Engineering | Volume 23 | Number 1 | September 1965 | Pages 8-20
Technical Paper | doi.org/10.13182/NSE65-A19254
Articles are hosted by Taylor and Francis Online.
Energy spectra were obtained experimentally for fission fragments escaping from backed films of enriched uranium dioxide that were less than 11 µm thick. The data were reduced to give values for the relative average escape energies (R), escape fractions (S) and energy deposition efficiencies (D). A mathematical model was developed to synthesize these results using a Monte-Carlo-type computer code. This code included the fission-fragment masses, yields, and initial energies, the experimental source-detector geometry, a range-energy relationship, an energy-loss relationship and a function for the pulse-height defect in surface-barrier detectors. Various functions for these last three parameters were used in combination to obtain results that duplicated the experimental spectra and R, S and D values. The agreement was obtained with range proportional to (energy)1/2, the square energy-loss function, and pulse-height defect = A (E) (M-B), where A and B are constants and E and M are energy and mass, respectively. The experimental detection functions were removed from the code, and the spectra and R, S and D values were calculated for a 2π geometry. These values agreed well with those calculated using weighted averages for range and initial energy.