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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. F. Zweifel, Joel H. Ferziger
Nuclear Science and Engineering | Volume 10 | Number 4 | August 1961 | Pages 357-361
doi.org/10.13182/NSE61-A15378
Articles are hosted by Taylor and Francis Online.
A “consistent P1” four-factor formula is derived. This formula, which contains an additional term not found in the usual four-factor formula, introduces a change in keff ∼ D2B2 where D is the thermal diffusion coefficient. The term is negative for hydrogen and positive for other moderators. The correction will be at most 1% Δk for a practical system. Since the four-factor formula is not expected to be accurate to 1%, it is proposed that this term be used mainly as a criterion for determining whether consistent P1 multigroup calculations are required, or whether simple group diffusion methods will suffice. By using the consistent P1 equations when the term D2B2 is of the order 1%, one will avoid the introduction of a consistent error into his reactor calculations. Finally, the consistent P1 multigroup equations are displayed, and it is seen that the procedure for their solution is not a great deal more difficult than for solving the usual multigroup equations.