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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.
James A. Grundl
Nuclear Science and Engineering | Volume 31 | Number 2 | February 1968 | Pages 191-206
Technical Paper | doi.org/10.13182/NSE68-A18231
Articles are hosted by Taylor and Francis Online.
The energy spectra of neutrons from the the thermal-neutron-induced fission of 235U, 233U, and 239Pu have been compared by means of eight activation detectors that cover the energy range 0.8 to 16 MeV. The detectors are exposed to fission neutrons produced at the center of a 10-cm-diam spherical cavity within a heavywater moderator. Comparison of detector responses for the three spectra yield average energy ratios, 235U: 233U: 239Pu = (1): (1.021 ± 0.005): (1.039 ± 0.002). Differences between the normalized spectra are most pronounced at high energies as exemplified by the relative 239Pu: 235U flux ratios 1.17 for 6 < E < 11 MeV and 1.35 for E > 11 MeV. Spectral indexes for the 235U fission spectrum, based on measurements with monoenergetic neutrons, show progressively fewer neutrons above 6 MeV than given by the usual Maxwellian description of the fission spectrum, χ235U(E) = (0.770)E1/2 exp (−0.775E). At lower energies, the observed spectral indexes involving the 235U, Np, and 238U fission detectors are significantly discrepant with those predicted.