Reduction of core-resonant m=1 magnetic fluctuations and improved confinement in the Madison Symmetric Torus [Dexter , Fusion Technol. 19, 131 (1991)] reversed-field pinch have been routinely achieved through control of the surface poloidal electric field, but it is now known that the achieved confinement has been limited in part by edge-resonant m=0 magnetic fluctuations. Now, through refined poloidal electric field control, plus control of the toroidal electric field, it is possible to reduce simultaneously the m=0 and m=1 fluctuations. This has allowed confinement of high-energy runaway electrons, possibly indicative of flux-surface restoration in the usually stochastic plasma core. The electron temperature profile steepens in the outer region of the plasma, and the central electron temperature increases substantially, reaching nearly 1.3 keV at high toroidal plasma current (500 kA). At low current (200 kA), the total beta reaches 15% with an estimated energy confinement time of 10 ms, a tenfold increase over the standard value which for the first time substantially exceeds the constant-beta confinement scaling that has characterized most reversed-field-pinch plasmas. (C) 2002 American Institute of Physics.

High confinement plasmas in the Madison Symmetric Torus reversed-field pinch

Marrelli L;
2002

Abstract

Reduction of core-resonant m=1 magnetic fluctuations and improved confinement in the Madison Symmetric Torus [Dexter , Fusion Technol. 19, 131 (1991)] reversed-field pinch have been routinely achieved through control of the surface poloidal electric field, but it is now known that the achieved confinement has been limited in part by edge-resonant m=0 magnetic fluctuations. Now, through refined poloidal electric field control, plus control of the toroidal electric field, it is possible to reduce simultaneously the m=0 and m=1 fluctuations. This has allowed confinement of high-energy runaway electrons, possibly indicative of flux-surface restoration in the usually stochastic plasma core. The electron temperature profile steepens in the outer region of the plasma, and the central electron temperature increases substantially, reaching nearly 1.3 keV at high toroidal plasma current (500 kA). At low current (200 kA), the total beta reaches 15% with an estimated energy confinement time of 10 ms, a tenfold increase over the standard value which for the first time substantially exceeds the constant-beta confinement scaling that has characterized most reversed-field-pinch plasmas. (C) 2002 American Institute of Physics.
2002
Istituto gas ionizzati - IGI - Sede Padova
Inglese
9
5
2061
2068
8
http://pop.aip.org/resource/1/phpaen/v9/i5/p2061_s1
Sì, ma tipo non specificato
Chapman, BE Almagri, AF Anderson, JK Biewer, TM Chattopadhyay, PK Chiang, CS Craig, D Den Hartog, DJ Fiksel, G Forest, CB Hansen, AK Holly, D Lanier, NE O'Connell, R Prager, SC Reardon, JC Sarff, JS Wyman, MD Brower, DL Ding, WX Jiang, Y Terry, SD Franz, P Marrelli, L Martin, P 43rd Annual Meeting of the Division of Plasma Physics of the American-Physical-Society Oct 29-nov 02, 2001 Long beach, california Amer Phys Soc, Div Plasma Phys 2. La rivista è pubblicata anche online con ISSN 1089-7674.
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info:eu-repo/semantics/article
262
Chapman, B E; Almagri, A F; Anderson, J K; Biewer, T M; Chattopadhyay, P K; Chiang, C S; Craig, D; Den Hartog, D J; Fiksel, G; Forest, C B; Hansen, A ...espandi
01 Contributo su Rivista::01.01 Articolo in rivista
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/204680
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