Local magnetic shear control in a tokamak via fast wave minority ion current drive : theory and experiments in jet

When an ion cyclotron resonance heating (ICRH) antenna array is phased ( Delta phi not=0 or pi ), the excited asymmetric k// spectrum can drive non-inductive currents by interaction of fast waves both with electrons (transit time magnetic pumping (e-TTMP) and Landau damping (e-LD)) and with ions at minority (fundamental) or harmonic cyclotron resonances, depending upon the scenario. On the basis of earlier theories, a simplified description is presented that includes the minority ion and electron current drive effects simultaneously in a 3-D ray tracing calculation in the tokamak geometry. The experimental results of sawtooth stabilization destabilization in JET using the minority ion current drive scheme are presented. This scheme allows a modification of the local current density gradient (or the magnetic shear) at the q=1 surface resulting in a control of sawteeth. The predictions of the above model of current drive and its effects on sawtooth period calculated in conjunction with a model of stability of internal resistive kink modes, that encompasses the effects of both the fast particle pressure and the local (q=1) magnetic shear, are found to be qualitatively in good agreement with the experimental results. Further, the results are discussed of our model of fast wave current drive scenarios of magnetic shear reversal with a view to achieving long duration high confinement regimes in the forthcoming experimental campaign on JET. Finally, the results are presented of minority current drive for sawtooth control in next step devices such as the International Thermonuclear Experimental Reactor (ITER)

[1]  Erwin Frederick Jaeger,et al.  Influence of various physics phenomena on fast wave current drive in tokamaks , 1993 .

[2]  Nathaniel J. Fisch Current generation by minority species heating , 1981 .

[3]  Tadashi Sekiguchi,et al.  Plasma Physics and Controlled Nuclear Fusion Research , 1987 .

[4]  V. Bhatnagar,et al.  Ray-tracing modelling of the ICRF heating of large tokamaks , 1984 .

[5]  Nathaniel J. Fisch,et al.  Theory of current-drive in plasmas , 1987 .

[6]  T. H. Stix Fast-wave heating of a two-component plasma , 1975 .

[7]  Bhatnagar,et al.  Stabilization of sawteeth with additional heating in the JET tokamak. , 1988, Physical review letters.

[8]  R. Prater,et al.  Current driven by asymmetrical minority heating in ICRF , 1983 .

[9]  D. Goodman Two‐dimensional plasma‐electron temperature measurements , 1989 .

[10]  V. Bhatnagar,et al.  A 3-D analysis of the coupling characteristics of ion cyclotron resonance heating antennae , 1982 .

[11]  G. Magyar,et al.  Plasma diagnostics on large tokamaks , 1988 .

[12]  J. Jacquinot,et al.  Radio-frequency heating system , 1987 .

[13]  E. Westerhof Tearing mode stabilization by local current density perturbations , 1990 .

[14]  P. Mantica,et al.  Experimental identification of Tokamak equilibrium using magnetic and diamagnetic signals , 1988 .

[15]  Tihiro Ohkawa,et al.  New methods of driving plasma current in fusion devices , 1970 .

[16]  M. Porkolab,et al.  Theory of fast wave current drive for tokamak plasmas , 1989 .

[17]  Charles F. F. Karney,et al.  Approximate formula for radiofrequency current drive efficiency with magnetic trapping , 1991 .

[18]  D.F.H. Start,et al.  Shear Reversal and Mhd Activity During Pellet Enhanced Performance Pulses in Jet , 1992 .

[19]  R. Granetz,et al.  JET Soft X-Ray Diode Array Diagnostic , 1986 .

[20]  D. Moreau,et al.  CONFERENCES AND SYMPOSIA: Fast wave current drive in reactor scale tokamaks , 1992 .

[21]  J. G. Cordey,et al.  Effects of neutral injection heating upon toroidal equilibria , 1974 .