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Conference Spotlight
Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Fusion Science and Technology
August 2025
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The newest era of workforce development at ANS
As most attendees of this year’s ANS Annual Conference left breakfast in the Grand Ballroom of the Chicago Downtown Marriott to sit in on presentations covering everything from career pathways in fusion to recently digitized archival nuclear films, 40 of them made their way to the hotel’s fifth floor to take part in the second offering of Nuclear 101, a newly designed certification course that seeks to give professionals who are in or adjacent to the industry an in-depth understanding of the essentials of nuclear energy and engineering from some of the field’s leading experts.
Wayne R. Meier
Fusion Science and Technology | Volume 3 | Number 3 | May 1983 | Pages 385-391
Technical Paper | Blanket Engineering | doi.org/10.13182/FST83-A20862
Articles are hosted by Taylor and Francis Online.
Monte Carlo neutronics calculations have been carried out to compare the effects of chamber ports on the neutron leakage and blanket performance for lithium and lead-lithium blankets. A spherical chamber with diametrically opposed, conical penetrations through the blanket and a 14.1-MeV point source at its center is the basis for the comparison. The total neutron leakage through ports in a lithium blanket is about two times greater than one would estimate based on the solid angle fraction subtended by the holes. For a blanket comprised primarily of the lead-lithium eutectic, Pb83Li17, the leakage per deuterium-tritium neutron is about six times the subtended solid angle fraction. As a result of the enhanced neutron leakage, the tritium-breeding ratio and neutron energy deposited in the blanket decrease more rapidly than the loss of blanket coverage. For example, for a chamber in which the ports subtend 5% of the total solid angle, the tritium-breeding ratios are ∼s and ∼20% less than the results without ports for the lithium and Pb83Li17 blankets, respectively. The neutron energy deposited in the blanket decreases ∼7% for lithium and ∼14% for Pb83Li17 for the same 5% loss in blanket coverage.