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2025 ANS Winter Conference & Expo
November 9–12, 2025
Washington, DC|Washington Hilton
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Researchers use one-of-a-kind expertise and capabilities to test fuels of tomorrow
At the Idaho National Laboratory Hot Fuel Examination Facility, containment box operator Jake Maupin moves a manipulator arm into position around a pencil-thin nuclear fuel rod. He is preparing for a procedure that he and his colleagues have practiced repeatedly in anticipation of this moment in the hot cell.
R. S. Massey, R. G. Watt, P. G. Weber, G. A. Wurden, D. A. Baker, C. J. Buchenauer, L. C. Burkhardt, T. Cayton, J. N. DiMarco, J. N. Downing, R. M. Erickson, R. F. Gribble, A. Haberstich, R. B. Howell, J. C. Ingraham, E. M. Little, G. Miller, C. P. Munson, J. A. Phillips, M. M. Pickrell, K. F. Schoenberg, A. E. Schofield, D. M. Weldon
Fusion Science and Technology | Volume 8 | Number 1 | July 1985 | Pages 1571-1580
Alternative Concept | Proceedings of the Sixth Topical Meeting on the Technology of Fusion Energy (San Francisco, California, March 3-7, 1985) | doi.org/10.13182/FST85-A39985
Articles are hosted by Taylor and Francis Online.
The present status of research on the ZT-40M Reversed-Field Pinch (RFP) will be described. RFP discharges have been sustained for times (27 ms) >> the classical resistive diffusion time, implying the existence of a flux-sustainment mechanism (“dynamo”). This mechanism opens the possibility for a steady-state RFP reactor utilizing a unique form of non-inductive current drive. Te > 500 eV has been obtained for 400 kA aischarges with ∼ 4 × 1019 m−3. Total energy confinement time τE has reached 0.7 ms with a Lawson parameter of 5 × 1016 m−3 s for discharges with = 8×1019 m−3 and Te = 330 eV at a plasma current of 330 kA and 0.33 T total confining field at the wall. Reactor-like βθ ∼ 10–20% is routinely obtained for plasma currents from 60–400 kA (β ∼ βθ/2). Scaling of τE ∼ I(2.2±0.4) is found, more than adequate for a compact RFP reactor.