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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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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The 2025 edition is a reinvigoration of the withdrawn ANS-54.8-1988 of the same title.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.
W. B. Doub
Nuclear Science and Engineering | Volume 10 | Number 4 | August 1961 | Pages 299-307
doi.org/10.13182/NSE61-A15371
Articles are hosted by Taylor and Francis Online.
An approximate heuristic expression for the particle self-shielding factor for a set of purely absorbing spheres of radius r and volume fraction V well mixed with another set of non-absorbing spheres has been derived. The resulting expression has been experimentally verified using transmission data at several incident neutron energies for a plate-type sample containing a mixture of aluminum and boron-carbide spheres with nominal diameters 85 ± 15µ. The boron-carbide spheres occupied about 37% of the sample volume. The transmission was measured at energies ranging from 0.03 to 1.2 ev using a crystal neutron spectrometer. Since, however, the sample contained boron-carbide spheres with a distribution of diameters, the experimental self-shielding factors are “average” values. It is shown, using an approximate model, that a plausible theoretical self-shielding factor is a volume weighted average of the self-shielding factors for the spheres of diameters, d1, d2, d3, … . The particle self-shielding factors derived by several other authors have also been compared with the present experimental results. The Hurwitz-Zweifel expression (1) gives quite bad agreement, though this is expected because of the high volume fraction of poison in the sample. The Burrus expression (2, 3) gives much better agreement though not as good as the expression derived in this paper.