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Status of the ZT-40M RFP Experimental Program

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 1P2B / 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) / dx.doi.org/10.13182/FST85-A39985

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.