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Fusion energy: Progress, partnerships, and the path to deployment
Over the past decade, fusion energy has moved decisively from scientific aspiration toward a credible pathway to a new energy technology. Thanks to long-term federal support, we have significantly advanced our fundamental understanding of plasma physics—the behavior of the superheated gases at the heart of fusion devices. This knowledge will enable the creation and control of fusion fuel under conditions required for future power plants. Our progress is exemplified by breakthroughs at the National Ignition Facility and the Joint European Torus.
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.