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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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A new ANSI/ANS standard for liquid metal fire protection published
ANSI/ANS-54.8-2025, Liquid Metal Fire Protection in LMR Plants, received approval from the American National Standards Institute on September 2 and is now available for purchase.
The 2025 edition is a reinvigoration of the withdrawn ANS-54.8-1988 of the same title. The Advanced Reactor Codes and Standards Collaborative (ARCSC) identified the need for a current version of the standard via an industry survey.
Typical liquid metal reactor designs use liquid sodium as the coolant for both the primary and intermediate heat-transport systems. In addition, liquid sodium and NaK (a mixture of sodium and potassium that is liquid at room temperature) are often used in auxiliary heat-removal systems. Since these liquid metals can react readily with oxygen, water, and other compounds, special precautions must be taken in the design, construction, testing, and maintenance of the sodium/NaK systems to ensure that the potential for leakage is very small.
R. D. Jain
Nuclear Science and Engineering | Volume 17 | Number 4 | December 1963 | Pages 551-556
Technical Paper | doi.org/10.13182/NSE63-A18447
Articles are hosted by Taylor and Francis Online.
The asymptotic energy spectrum of thermal neutrons in an infinite medium of beryllium has been calculated for three temperatures: 300°K, 200°K, 100°K, for a constant plane source of neutrons at the midplane. The techniques of multigroup diffusion theory were applied, using Nelkin's first order scattering kernel for Be, and the energy-dependent transport mean free path, λtr(E), calculated by Bhandari. Because of the violent variation of λtr in the vicinity of the Bragg cutoff energy, for the lower moderator temperatures the calculated flux spectrum is quite different from the Maxwellian. At 300°K the deviation from the Maxwellian is small.