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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.”
S. Danani, Hitesh Kumar B. Pandya, P. Vasu, M. E. Austin
Fusion Science and Technology | Volume 59 | Number 4 | May 2011 | Pages 651-656
Technical Paper | Sixteenth Joint Workshop on Electron Cyclotron Emission and Electron Cyclotron Resonance Heating (EC-16) | doi.org/10.13182/FST11-A11729
Articles are hosted by Taylor and Francis Online.
The electron cyclotron emission measurable from the outboard side of ITER plasmas is estimated. The effects of harmonic overlap and polarization scrambling are reviewed with the aim of assessing the impact of any polarization change that might occur in the collected radiation before the O and X polarizations are separated. It is confirmed that any polarization scrambling occurring during the reflection at the wall would not alter the measured intensities of lower harmonics of either the O or X mode but would affect only the higher harmonics, which are optically thin. For the second-harmonic X mode, the observed intensity in the 300- to 400-GHz range is considerably lower than that of the O polarization. Hence, this frequency range may be particularly vulnerable to any O-to-X polarization change occurring prior to their separation into different transmission channels. It is shown that if the electron temperature Te near the core is to be measured to within 10% accuracy, the above polarization fidelity should also be preserved to within 10% or better. It is suggested that this requirement may have impact on the location of the polarization splitter unit. Further analysis is required to evaluate the error in the calculation of Te profiles from the measured Trad values arising due to uncertainties introduced by any polarization conversion.