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The Radiation Protection and Shielding Division is developing and promoting radiation protection and shielding aspects of nuclear science and technology — including interaction of nuclear radiation with materials and biological systems, instruments and techniques for the measurement of nuclear radiation fields, and radiation shield design and evaluation.
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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Latest News
Take steps on SNF and HLW disposal
Matt Bowen
With a new administration and Congress, it is time once again to ponder what will happen—if anything—on U.S. spent nuclear fuel and high-level waste management policy over the next few years. One element of the forthcoming discussion seems clear: The executive and legislative branches are eager to talk about recycling commercial SNF. Whatever the merits of doing so, it does not obviate the need for one or more facilities for disposal of remaining long-lived radionuclides. For that reason, making progress on U.S. disposal capabilities remains urgent, lest the associated radionuclide inventories simply be left for future generations to deal with.
In March, Rick Perry, who was secretary of energy during President Trump’s first administration, observed that during his tenure at the Department of Energy it became clear to him that any plan to move SNF “required some practical consent of the receiving state and local community.”1
Kaname Kizu, Keiji Miyazaki, Tetsuo Tanabe
Fusion Science and Technology | Volume 28 | Number 3 | October 1995 | Pages 1205-1210
Tritium Properties and Interaction with Material | Proceedings of the Fifth Topical Meeting on Tritium Technology In Fission, Fusion, and Isotopic Applications Belgirate, Italy May 28-June 3, 1995 | doi.org/10.13182/FST95-A30573
Articles are hosted by Taylor and Francis Online.
A precise hydrogen permeation experiment for beryllium was conducted at a temperature ranging from 735 to 1000 K under hydrogen gas pressure of 101 to 103 Pa. Diffusion coefficient and permeation coefficient were determined from the steady state penneation and time transient penneation independently. The steady state penneation rate was proportional to the square root of H2 pressure and the time sequence of penneation rate agreed well with theoretical one, indicating that the penneation controlled by bulk diffusion. The temperature dependencies of the penneation coefficients (Φ) and diffusion coefficients (D) were respectively,Φ=(1.0±0.1)×10−6exp[−73±20(kJ/mol)/RT] (mol·m−1·s−1·Pa1/2),D=(1.3±0.1)×10−7exp[59±20(kJ/mol)/RT] (m2·s−1).Solubility calculated from the relation Φ=DS wasS=7.1 exp[−14(kJ/mol)/RT] (mol·m−3·Pa−1/2).