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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.
Naphtali M. Mokgalapa, Tushar K. Ghosh, Sudarshan K. Loyalka
Nuclear Technology | Volume 186 | Number 1 | April 2014 | Pages 45-59
Technical Paper | Reactor Safety | doi.org/10.13182/NT13-9
Articles are hosted by Taylor and Francis Online.
In high-temperature gas reactors, graphite particle adhesion and resuspension from structural surfaces play a role in source term estimations. This paper describes measurements of the adhesion force between an irregular graphite cluster (henceforth called a graphite particle) and Hastelloy X samples having different surface conditions. An atomic force microscope (AFM) was used. The graphite particle was attached to the AFM probe and then brought directly into and out of contact with the surface in air; the adhesion force was obtained from the resultant force curve. The adhesion forces of the graphite particle with Hastelloy X (as received, polished, and different oxidations) and mica surfaces were determined. From the resulting adhesion forces, the work of adhesion W12 (energy per unit area) was calculated. Although the values of the measured pull-off (adhesion) forces were found to be of the same order of magnitude, they differed by surface condition depending where on the sample the adhesion force was measured. The theoretical value of the adhesion force was calculated using the theory of Johnson, Kendall, and Roberts. When compared to the values calcluated from this theory, the measured values were lower by a factor of 100 in some cases and 1000 in others. This difference may be due to the approximation of the irregular graphite cluster probe as a perfect graphite particle sphere and to not taking into consideration asperities on the surface of the particle probe. Additionally, covalent bonds may form between the surface elements and the graphite particle because of the applied load. In this paper, the effects of oxidation on the adhesion of graphite particles to the mica and Hastelloy X surfaces are also discussed.