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2025 ANS Winter Conference & Expo
November 9–12, 2025
Washington, DC|Washington Hilton
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Fusion Science and Technology
October 2025
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NN Asks: What did you learn from ANS’s Nuclear 101?
Mike Harkin
When ANS first announced its new Nuclear 101 certificate course, I was excited. This felt like a course tailor-made for me, a transplant into the commercial nuclear world. I enrolled for the inaugural session held in November 2024, knowing it was going to be hard (this is nuclear power, of course)—but I had been working on ramping up my knowledge base for the past year, through both my employer and at a local college.
The course was a fast-and-furious roller-coaster ride through all the key components of the nuclear power industry, in one highly challenging week. In fact, the challenges the students experienced caught even the instructors by surprise. Thankfully, the shared intellectual stretch we students all felt helped us band together to push through to the end.
We were all impressed with the quality of the instructors, who are some of the top experts in the field. We appreciated not only their knowledge base but their support whenever someone struggled to understand a concept.
Y. U. Nam
Fusion Science and Technology | Volume 55 | Number 2 | February 2009 | Pages 180-184
Technical Paper | Seventh International Conference on Open Magnetic Systems for Plasma Confinement | doi.org/10.13182/FST09-A7009
Articles are hosted by Taylor and Francis Online.
A 280 GHz single-channel horizontal millimeter-wave interferometer system has been installed for plasma electron density measurements on the Korea Superconducting Tokamak Advanced Research (KSTAR). An electron density of plasma is measured on double-path horizontal line with triangular geometry. A cassette system contains two vacuum windows was installed on median port for these purpose. Maximum line-integrated electron density of first plasma is set to 1019 m-2 in this geometry. Since a line density of single-fringe in 280 GHz is 2 × 1018 m-2, a multi-fringe counting circuit has been adopted for a fringe-jump compensation. Measured IF signals are divided into 4 channels which has fringe counting capability of 1, 2, 4 and 8 fringes, respectively. A phase difference between IF signals is converted to DC voltage in each channel according to its fringe coverage. A fringe-jump analysis algorism has been developed for a discrimination of real fringe-jump from noise signal. An electron density of the KSTAR first plasma has been measured and analyzed using this system. Upon these results, an advanced fringe counting scheme will be proposed in this paper.