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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. C. Hanna
Nuclear Science and Engineering | Volume 15 | Number 3 | March 1963 | Pages 325-337
Technical Paper | doi.org/10.13182/NSE63-A26444
Articles are hosted by Taylor and Francis Online.
Skyrme has given a theoretical treatment of the perturbation of the neutron flux in a diffusing medium by an absorbing foil. His theory is re-examined, with particular reference to the modification proposed by Ritchie and Eldridge, and the “edge correction” is evaluated. The accuracy of this modified Skyrme theory is tested by comparison with Dalton and Osborn’s computer calculations for monokinetic neutrons; the agreement is generally better than 1%. This theory is then extended to a Maxwellian neutron spectrum, for which computer calculations are not available, with the result
A is the activity per unit mass of a foil of thickness τ (in units of the absorption mean free path), Ao that of a zero thickness foil, , where t and R are the thickness and radius of the foil. The bars denote averages over the Maxwellian spectrum. The flux-depression parameter g is of the order of R/λtr, but its exact value depends on the velocity dependence of the transport mean free path, and on the thermalization properties of the medium. This formula is used to obtain, from the available measurements of the dependence of A on foil thickness, “experimental” values of g. For both graphite and hydrogenous media they are smaller than expected.