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NIMROD calculations of energetic particle driven toroidal Alfvén eigenmodes
Toroidal Alfvén eigenmodes (TAEs) are gap modes induced by the toroidicity of tokamak plasmas in the absence of continuum damping. They can be excited by energetic particles (EPs) when the EP drive exceeds other dampings, such as electron and ion Landau damping, and collisional and radiative damping...
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Published in: | Physics of plasmas 2018-01, Vol.25 (1) |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Toroidal Alfvén eigenmodes (TAEs) are gap modes induced by the toroidicity of tokamak
plasmas in the absence of continuum damping. They can be excited by energetic particles
(EPs) when the EP drive exceeds other dampings, such as electron and ion Landau damping,
and collisional and radiative damping. A TAE benchmark case, which was proposed by the
International Tokamak Physics Activity group, is studied in this work. The numerical
calculations of linear growth of TAEs driven by EPs in a circular-shaped, large aspect
ratio tokamak have been performed using the Hybrid Kinetic-MHD (HK-MHD) model implemented
in the NIMROD code. This HK-MHD model couples a δf
particle-in-cell representation of EPs with the 3D MHD representation of the bulk plasma
through moment closure for the momentum conservation equation. Both the excitation of TAEs
and their transition to energetic particle modes (EPMs) have been observed. The influence
of EP density, temperature, density gradient, and position of the maximum relative density
gradient, on the frequency and the growth rate of TAEs are obtained, which are consistent
with those from the eigen-analysis calculations, kinetic-MHD, and gyrokinetic simulations
for an initial Maxwellian distribution of EPs. The relative pressure gradient of EP at the
radial location of the TAE gap, which represents the drive strength of EPs, can strongly
affect the growth rate of TAEs. It is demonstrated that the mode transition due to EP
drive variation leads to not only the change of frequency but also the change of the mode
structure. This mechanism can be helpful in understanding the nonlinear physics of
TAE/EPM, such as frequency chirping. |
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ISSN: | 1070-664X 1089-7674 |
DOI: | 10.1063/1.4999619 |