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Conference Spotlight
Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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U.S. nuclear supply chain: Ready for liftoff
Craig Piercycpiercy@ans.org
This month, September 8–11, the American Nuclear Society is teaming up with the Nuclear Energy Institute to host our first-ever Nuclear Energy Conference and Expo—NECX for short—in Atlanta. This new meeting combines ANS’s Utility Working Conference and NEI’s Nuclear Energy Assembly to form what NEI CEO Maria Korsnick and I hope will be the premier nuclear industry gathering in America.
We did this because after more than four decades of relative stagnation, the U.S. nuclear supply chain is finally entering a new era of dynamic growth. This resurgence is being driven by several powerful and increasingly durable forces: the explosive demand for electricity from artificial intelligence and data centers, an unprecedented wave of public and private acceptance of—and investment in—advanced nuclear technologies, and a strong market signal for reliable, on-demand power. Add the recent Trump administration executive orders on nuclear into the mix, and you have all the makings of an accelerant-rich business environment primed for rapid expansion.
Takashi Hosoma, Masanori Aritomi, Tsunemichi Kawa
Nuclear Technology | Volume 120 | Number 2 | November 1997 | Pages 121-135
Technical Paper | Enrichment and Reprocessing System | doi.org/10.13182/NT97-A35421
Articles are hosted by Taylor and Francis Online.
Bubble shape and excess pressure in dip-tube pressure measurement for density, level, and volume determination of plutonium nitrate solution in a reprocessing and plutonium conversion plant are studied theoretically and experimentally because the excess pressure is a source of error for highly accurate materials accounting. The bubble shape calculated numerically at equilibrium has a convex face above, like the upper part of a torus. The excess pressure is calculated from liquid density, surface tension, and the torus diameter, without the bottom curvature and height of the bubble. The excess pressure reaches a maximum when the torus diameter reaches the inner diameter of the tube. The bubble breaks and excess pressure reaches a minimum just after the bubble surface reaches the outer surface of the tube. The excess pressure is independent of liquid level and bubbling frequency, if the frequency is less than once every 5 s.