A. Pochelon, S. Alberti, C. Angioni,
S. Barry, R. Behn, P. Blanchard, P. Bosshard,
R. Chavan, S. Coda, B. P. Duval, D. Fasel,
A. Favre, S. Franke, I. Furno, T. P. Goodman,
P. Gorgerat, M. Henderson, F. Hofmann, J-P. Hogge,
P-F. Isoz, B. Joye, J. B. Lister, X. Llobet,
J-C. Magnin, P. Mandrin, A. Manini, B. Marletaz,
Ph. Marmillod, Y. Martin, J-M. Mayor, J-M. Moret,
Ch. Nieswand, P. J. Paris, A. Perez, Z. A. Pietrzyk,
R. A. Pitts, A. Refke, H. Reimerdes, J. Rommers,
O. Sauter, W. van Toledo, G. Tonetti, M. Q. Tran,
F. Troyon, P. Vyas, H. Weisen
Centre de Recherches en Physique des Plasmas, Association EURATOM -
Confédération Suisse, Ecole Polytechnique Fédérale de Lausanne,
CH-1015 Lausanne, Switzerland
Yu. V. Esipchuck, N. Kirneva, A. A. Martynov,
K. A. Razumova, A. Sushkov
Institute of Nuclear Fusion, Russian Research Centre, Kurchatov
Institute, 123 182 Moscow, Russia
F. Porcelli, E. Rossi
Dipartimento Di Energetica Politecnico di Torino I-10129 Torino,
Italy
Abstract. Confinement in TCV (Tokamak à Configuration Variable) EC heated
discharges is studied as a function of plasma shape, i.e. as a function of
elongation
1.1 < kappa < 2.15 and triangularity
-0.65 0.5. The electron energy confinement time is found to increase with
elongation, in part due to the increase of plasma current with elongation. The
beneficial effect of negative triangularities is most effective at low power
and tends to reduce at the higher powers used. The large variety of sawtooth
types observed in TCV for different power deposition locations from on axis to
the q = 1 region can be simulated with a model including a local power
deposition, a growing m/n = 1 island (convection and reconnection), plasma
rotation and finite heat diffusivity across flux surfaces.
IAEA 2001