An investigation of beam driven Alfvén instabilities in the DIII-D tokamak

Neutral beams were injected into low field (B = 0.7-1.0 T) deuterium plasmas in an attempt to destabilize toroidicity induced Alfven eigenmodes (TAE modes). When the parallel beam velocity approached the Alfven velocity and the volume averaged beam beta exceeded 2%, localized, propagating modes with n = 2-10 were observed. As much as 45% of the beam power was lost as a result of the modes. The threshold for TAE instability is at least one order of magnitude higher than that predicted by Fu and VanDam (Phys. Fluids B 1 (1989) 1949).

[1]  R. White,et al.  Alpha‐particle losses from toroidicity‐induced Alfvén eigenmodes. Part II: Monte Carlo simulations and anomalous alpha‐loss processes , 1992 .

[2]  J. Whitson,et al.  Destabilitization of low mode number Alfvén modes in a tokamak by energetic or alpha particles , 1981 .

[3]  W. Tang,et al.  Measurements and implications of Zeff profiles on the DIII‐D tokamak , 1988 .

[4]  D. Spong,et al.  Destabilization of tokamak pressure-gradient driven instabilities by energetic alpha-particle populations , 1990 .

[5]  J. Haskovec,et al.  Toroidal and poloidal soft x-ray imaging system on the DIII-D tokamak , 1988 .

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

[7]  C. Cheng,et al.  Alpha-particle effects on low-n magnetohydrodynamic modes , 1990 .

[8]  T. Lehecka,et al.  Reflectometry systems for the DIII-D tokamak , 1988 .

[9]  E. Doyle,et al.  Far‐infrared heterodyne scattering to study density fluctuations on the DIII‐D tokamak , 1990 .

[10]  J. L. Luxon,et al.  Big Dee - A Flexible Facility Operating Near Breakeven Conditions , 1985 .

[11]  P. Gohil,et al.  Multipoint Thomson scattering diagnostic for DIII-D , 1988 .

[12]  L. Lao,et al.  Reconstruction of current profile parameters and plasma shapes in tokamaks , 1985 .

[13]  H. Takeuchi,et al.  Magnetohydrodynamic activity in the JFT-2 tokamak with high-power neutral-beam-injection heating , 1981 .

[14]  Paul,et al.  Excitation of toroidal Alfvén eigenmodes in TFTR. , 1991, Physical review letters.

[15]  H. Kugel,et al.  Studies of energetic ion confinement during fishbone events in PDX , 1985 .

[16]  W. Heidbrink,et al.  The fishbone instability in the DIII-D tokamak , 1990 .

[17]  M. S. Chance,et al.  Low-n shear Alfven spectra in axisymmetric toroidal plasmas , 1986 .

[18]  G. Fu,et al.  Stability of the global Alfvén eigenmode in the presence of fusion alpha particles in an ignited tokamak plasma , 1989 .

[19]  K. Burrell,et al.  Multichordal visible/near‐UV spectroscopy on the DIII‐D tokamak , 1988 .

[20]  Chio Cheng,et al.  Alpha particle destabilization of the toroidicity-induced Alfvén eigenmodes , 1991 .

[21]  H. R. Hicks,et al.  Magnetohydrodynamic instability with neutral-beam heating in the ISX-Beta tokamak , 1982 .

[22]  A. Nishida Magnetospheric plasma physics. , 1982 .

[23]  G. Fu,et al.  Theory of a high‐n toroidicity‐induced shear Alfvén eigenmode in tokamaks , 1990 .

[24]  D. McCune,et al.  Charge exchange measurements of MHD activity during neutral beam injection in the Princeton Large Torus and the Poloidal Divertor Experiment , 1987 .

[25]  J. W. Van Dam,et al.  Excitation of the toroidicity-induced shear Alfvén eigenmode by fusion alpha particles in an ignited tokamak , 1989 .

[26]  J. Weiland,et al.  Magnetohydrodynamic ballooning instabilities excited by energetic trapped particles , 1985 .

[27]  W. Heidbrink The DIII-D EpB charge exchange diagnostic , 1988 .

[28]  R. Groebner,et al.  Comparison of experimental and theoretical fast ion slowing-down times in DIII-D , 1988 .

[29]  G. Hammett,et al.  Measurements of beam‐ion confinement during tangential beam‐driven instabilities in a bean tokamak experiment , 1987 .

[30]  Takahashi,et al.  Tangential neutral-beam-driven instabilities in the Princeton beta experiment. , 1986, Physical review letters.

[31]  W. Heidbrink Neutron fluctuation measurements on TFTR , 1986 .

[32]  Yan Ming Li,et al.  Destabilization of global Alfvén eigenmodes and kinetic Alfvén waves by alpha particles in a tokamak plasma , 1987 .

[33]  J. P. Goedbloed Spectrum of ideal magnetohydrodynamics of axisymmetric toroidal systems , 1975 .

[34]  Microinstability theory of two-energy-component toroidal systems , 1975 .

[35]  H. Neilson,et al.  Fast ion confinement during high power tangential neutral beam injection into low plasma current discharges on the ISX-B tokamak , 1988 .

[36]  Liu Chen,et al.  Theory of energetic trapped particle-induced resistive interchange-ballooning modes , 1986 .

[37]  M. N. Rosenbluth,et al.  Excitation of Alfven waves by high-energy ions in a tokamak , 1975 .