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Conference Spotlight
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The 2025 edition is a reinvigoration of the withdrawn ANS-54.8-1988 of the same title.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.
V. E. Schrock, L. M. Grossman
Nuclear Science and Engineering | Volume 12 | Number 4 | April 1962 | Pages 474-481
Technical Paper | doi.org/10.13182/NSE62-A26094
Articles are hosted by Taylor and Francis Online.
Local heat transfer coefficients and pressure gradients have been measured for bulk boiling of water in forced flow (vertically upward) in round tubes with internal diameters ranging from 0.1162 to 0.4317 in., lengths of 15 to 40 in., heat fluxes of 6 × 104 to 1.45 × 106 Btu/hr ft2, mass fluxes of 49 to 911 lb/sec ft2, exit qualities of 5 to 57%, and at pressures ranging from 42 to 505 psia. The local heat transfer coefficients expressed in the form of the Nusselt number have been correlated in terms of Reynolds and Prandtl numbers and two dimensionless groups characterizing forced convection vaporization, the Lockhart-Martinelli parameter Xtt, and the “boiling number,” Bo = (q/A)/Ghfg. For large values of the latter, nucleate boiling predominates and the dependence of the heat transfer on Xtt is small. Conversely, at the small values of Bo, convective flow effects are dominant, and there is a strong dependence on Xtt.