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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.
G. P. Calame, F. D. Federighi
Nuclear Science and Engineering | Volume 10 | Number 2 | June 1961 | Pages 190-201
Technical Paper | doi.org/10.13182/NSE61-A25958
Articles are hosted by Taylor and Francis Online.
Knowledge of the spatially dependent thermal spectrum near an interface between different media is important for many reactor calculations. The Kantorovich variational method is utilized to solve the equation where the subscript n denotes the nth spatial region. A functional, J, of Φ(E, ) and of Φ+(E, ), is found such that the solutions to the equation and its adjoint make J stationary. Trial functions for Φ and Φ+ are employed which are linear combinations of the infinite medium spectra and adjoints, respectively, of a hard and a soft region. The constants of combination are undetermined functions of . These trial functions are inserted into J and the energy integrations performed. When the resulting expression is made stationary with respect to arbitrary variations of the adjoint constants of combination, there results in the nth region a set of two coupled differential equations for the flux constants of combination. The equations are solved simultaneously, yielding the energy spectrum as a function of position. The spectrum is used to obtain activation rates, and the rates are compared to experiments. The agreement is excellent. The method, that of overlapping groups, appears to be a promising one for the solution of the thermal space energy problem in more complex reactor calculations.