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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.
B. E. Simmons
Nuclear Science and Engineering | Volume 5 | Number 4 | April 1959 | Pages 254-256
Technical Paper | doi.org/10.13182/NSE59-A25593
Articles are hosted by Taylor and Francis Online.
A dynamic reactivity, not the reactivity in general use, is defined relative to prompt critical as ΔK = −lα, where α is the asymptotic (prompt) flux decay rate observed in a pulsed neutron experiment, and l is the prompt generation time of that same reactor made prompt critical by uniform subtraction of 1/υ poison. The dynamic reactivity coalesces near critical with the conventional perturbation reactivity δν/ν. The dynamic reactivity is physically interpretable as the amount of uniform 1/υ poison whose removal would result in criticality, times the conventional reactivity coefficient of that poison in the critical reactor. The quantity l has the physical significance of the average time taken by a neutron to cause a fission in the steady-state prompt-critical reactor; l is also the reactivity coefficient just mentioned.