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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Remembering ANS member Gil Brown
Brown
The nuclear community is mourning the loss of Gilbert Brown, who passed away on July 11 at the age of 77 following a battle with cancer.
Brown, an American Nuclear Society Fellow and an ANS member for nearly 50 years, joined the faculty at Lowell Technological Institute—now the University of Massachusetts–Lowell—in 1973 and remained there for the rest of his career. He eventually became director of the UMass Lowell nuclear engineering program. After his retirement, he remained an emeritus professor at the university.
Sukesh Aghara, chair of the Nuclear Engineering Department Heads Organization, noted in an email to NEDHO members and others that “Gil was a relentless advocate for nuclear energy and a deeply respected member of our professional community. He was also a kind and generous friend—and one of the reasons I ended up at UMass Lowell. He served the university with great dedication. . . . Within NEDHO, Gil was a steady presence and served for many years as our treasurer. His contributions to nuclear engineering education and to this community will be dearly missed.”
John R. McCarty, Michael J. Kolar
Nuclear Technology | Volume 29 | Number 3 | June 1976 | Pages 406-414
Technical Paper | Fusion Reactor Material / Reactor | doi.org/10.13182/NT76-A31605
Articles are hosted by Taylor and Francis Online.
Containment design pressure for a high-temperature gas-cooled reactor is determined by its response to a design basis depressurization accident. The effects of heat transfer to internal structures and of helium mixing significantly affect the response. In the mathematical model, the containment is divided into two regions; a lower region that contains only air, and an upper region that contains all the helium and whatever air is assumed to mix. Heat sinks are distributed vertically. At each instant, a given heat sink is calculated to be in either the unmixed region or the mixed region. In this way, both the mixing fraction and the heat transfer data can be changed. The peak pressure can be reduced by (a) placing heat sinks higher in the containment, (b) increasing the mixing fraction, and (c) accounting for heat transfer as the helium rises through the lower region.