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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.
Rouyentan Farhadieh
Nuclear Science and Engineering | Volume 77 | Number 1 | January 1981 | Pages 84-91
Technical Paper | doi.org/10.13182/NSE81-A21341
Articles are hosted by Taylor and Francis Online.
An experimental study of the melting of a vertical surface of a solid by a heated liquid pool of various densities was conducted. The heat transfer mode in the external fluid was by natural turbulent thermal convection. After the onset of melting, although the two media were miscible, the melt and external fluid did not intermix along their mutual vertical interface when densities of the two media were different. The melt flowed upward when the liquid pool was heavier, and downward otherwise. For these cases, the heat transfer to the solid surface was controlled by the flow of the melt layer. As the density of the liquid pool approached that of the melt, the melting rate decreased, assuming a minimum at a liquid-melt density ratio, ρ*, of about one. For ρ* < 1.1, the convective currents within the liquid pool became increasingly effective in the removal of the melt. The mixing of the two media increased, with maximum mixing occurring at ρ* ≈ 1. For this case, convection currents in the liquid pool became the controlling heat transfer mechanism.