Published December 1, 2017 | Version v1
Journal article

Analysis of Alfven eigenmodes destabilization by energetic particles in TJ-II using a Landau-closure model

  • 1. Oak Ridge National Laboratory, Oak Ridge, TN 37831-8071 (United States)
  • 2. Universidad Carlos III de Madrid, 28911 Leganes, Madrid (Spain)

Description

Alfvén Eigenmodes (AE) can be destabilized by energetic particles in neutral beam injection (NBI) heated plasmas through inverse Landau damping and couplings with gap modes in the shear Alfvén continua. We describe the linear evolution of the poloidal flux and the toroidal component of the vorticity in a full 3D system using the reduced MHD equations, density and parallel velocity moments for the energetic particles as well as the geodesic acoustic wave dynamics. A closure relation adds the Landau damping and resonant destabilization effects in the model. We apply the model to study the Alfvén modes stability in TJ-II, performing a parametric analysis in a range of realistic values of energetic particle β ( β f ), ratios of thermal/Alfvén velocities ( V t h / V A 0 ), energetic particle density profiles and toroidal modes (n) including toroidal and helical couplings. The study predicts a large helical coupling between different toroidal modes and the destabilization of helical Alfvén eigenmodes (HAE) with frequencies similar to the AE activity measured in TJ-II, between 50–400 kHz. The analysis has also revealed the destabilization of GAE (global Alfvén eigenmodes), TAE (toroidal Alfvén eigenmodes) and EPM (energetic particle modes). For the modes considered here, optimized TJ-II operations require a ι profile in the range of [ 0.845 , 0.979 ] to stabilize AEs in the inner and middle plasma. AEs in the plasma periphery cannot be fully stabilized, although for a configuration with ι = [ 0.945 , 1.079 ], only n = 7 , 11 , 15 AE are unstable with a growth rate 4 times smaller compared to the standard ι = [ 1.54 , 1.68 ] case and a frequency of 100 kHz. We reproduce the frequency sweeping evolution of the AE frequency observed in TJ-II as the ι profile is varied. The AE frequency sweeping is caused by consecutive changes of the instability dominant modes between different helical families. (paper)

Availability note (English)

Available from http://dx.doi.org/10.1088/1741-4326/aa83c4

Additional details

Identifiers

Publishing Information

Journal Title
Nuclear Fusion
Journal Volume
57
Journal Issue
12
Journal Page Range
[14 p.]
ISSN
0029-5515
CODEN
NUFUAU

INIS

Country of Publication
International Atomic Energy Agency (IAEA)
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
51089849
Subject category
S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
Descriptors DEI
AUGER ELECTRON SPECTROSCOPY; BEAM INJECTION; COUPLINGS; LANDAU DAMPING; PARAMETRIC ANALYSIS; PARTICLES; PLASMA; SOUND WAVES
Descriptors DEC
DAMPING; ELECTRON SPECTROSCOPY; SPECTROSCOPY