Combined heating experiments in ELM-free H modes in JET

High power combined NBI + ICRF heating experiments have been carried out in the JET Mark IIa divertor configuration in the hot ion ELM-free H mode regime, both in deuterium (DD) and in deuterium-tritium (DT) plasmas. Results are presented from a wide range of additional heating power levels, ICRF up to 9.5 MW tuned to the fundamental hydrogen minority, NBI up to 22 MW, and for plasma currents up to 4.2 MA and toroidal fields up to 3.6 T. Discharges with combined NBI + ICRF heating show a clear improvement in electron temperature, DD neutron yield and stored energy with respect to NBI only discharges. High energy neutral particle analyser data show that acceleration of the NBI deuterons takes place due to absorption of ICRF power at the second harmonic deuterium resonance. This is confirmed by numerical simulations with the PION code, indicating that up to 40% of the ICRF power is absorbed by bulk and NBI ions. ICRF heating has been an essential ingredient in the DT experiments in the ELM-free hot ion regime, contributing to the achievement of a record fusion power of 16.1 MW and a record stored energy of 17 MJ.

[1]  F. G. Rimini,et al.  Observation of Alpha Heating in JET DT Plasmas , 1998 .

[2]  R. König,et al.  An overview of MHD activity at the termination of JET hot ion H modes , 1997 .

[3]  J. Jacquinot Heating, current drive and confinement regimes with the JET ICRH and LHCD systems , 1991 .

[4]  T. H. Stix,et al.  Heating of toroidal plasmas by neutral injection , 1972 .

[5]  J. Pain Plasma Physics , 1968, Nature.

[6]  W. Kerner,et al.  High fusion performance from deuterium-tritium plasmas in JET , 1999 .

[7]  3He-d fusion reaction rate measurements during ICRH heating experiments in JET , 1989 .

[8]  J. Lister,et al.  Alfven eigenmode experiments in tokamaks and stellarators , 1997 .

[9]  F. G. Rimini,et al.  D-T fusion with ion cyclotron resonance heating in the JET tokamak , 1998 .

[10]  B. Alper,et al.  Identification of external kink modes in JET , 1998 .

[11]  Jet Team,et al.  Fusion energy-production from a deuterium-tritium plasma in the jet tokamak , 1992 .

[12]  A. Gondhalekar,et al.  Impurity induced neutralization of megaelectronvolt energy protons in JET plasmas , 1997 .

[13]  F. Rimini,et al.  ICRF Heating of JET Plasmas with the Third-Harmonic Deuterium Resonance , 1998 .

[14]  Theory of alfvén eigenmode instabilities and related alpha particle transport in JET deuterium-tritium plasmas , 1998 .

[15]  M. V. Hellermann,et al.  Edge transport barrier in JET hot ion H modes , 2000 .

[16]  Miss A.O. Penney (b) , 1974, The New Yale Book of Quotations.

[17]  T. Hellsten,et al.  Comparison of time dependent simulations with experiments in ion cyclotron heated plasmas , 1993 .

[18]  Kenneth M. Young,et al.  Diagnostics for experimental thermonuclear fusion reactors , 1996 .

[19]  James R. Wilson,et al.  Ion cyclotron range of frequencies heating and current drive in deuterium–tritium plasmas , 1995 .

[20]  J. Cordey,et al.  Heat transport with strong off-axis heating , 1992 .

[21]  R. König,et al.  Analysis of bulk ion heating with ICRH in JET high-performance plasmas , 1999 .

[22]  V. Parail,et al.  Profile control experiments in JET using off-axis lower hybrid current drive , 1998 .