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Conference Spotlight
2025 ANS Winter Conference & Expo
November 9–12, 2025
Washington, DC|Washington Hilton
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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.
G. L. Jackson, M. E. Austin, J. S. deGRASSIE, A. W. Hyatt, J. M. Lohr, T. C. Luce, R. Prater, W. P. West
Fusion Science and Technology | Volume 57 | Number 1 | January 2010 | Pages 27-40
Technical Paper | doi.org/10.13182/FST10-A9266
Articles are hosted by Taylor and Francis Online.
Second-harmonic X-mode (X2) electron cyclotron (EC) heating (ECH) has been used in DIII-D in conjunction with plasma initiation and current ramp-up. Although the toroidal inductive electric field E in DIII-D is high enough (0.9 to 1.0 V/m) to allow robust start-up without EC assist, start-up in fusion devices such as ITER will have lower fields (E = 0.3 V/m), and EC assist can provide a reproducible breakdown and an increased margin for burnthrough of low-Z impurities. ECH, applied before the inductive electric field, is used to separate the various phases of plasma breakdown and start-up and is defined as preionization. Preionization first occurs near the X2 resonance location and then expands in the vessel volume. Perpendicular launch (k[parallel] = 0) is found to produce the strongest preionization. The power threshold for preionization can be reduced by optimizing the prefill and the vertical field, although the lowest power threshold is not at the optimum value for ohmic start-up alone. An orbit-following code confirms that cold electrons (0.03 eV) can be sufficiently heated by ECH to energies above the threshold of ionization of hydrogen. This code predicts heating in new tokamaks such as KSTAR and ITER to energies where preionization can occur. The ITER start-up scenario has been simulated in DIII-D experiments, and X2 ECH assist has been applied at reduced toroidal loop voltage to assist burnthrough and plasma current ramp-up.