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Theory of continuum damping of toroidal Alfven eigenmodes in finite-[beta] tokamaks

Journal Article · · Physics of Fluids B; (United States)
DOI:https://doi.org/10.1063/1.860839· OSTI ID:6022147
;  [1]
  1. Plasma Physics Laboratory and Department of Astrophysical Sciences, Princeton University, Princeton, New Jersey 08543 (United States)

A general theoretical approach has been formulated for analyzing two-dimensional structures of high-[ital n] toroidal Alfven eigenmodes (TAE) in large aspect-ratio, finite-[beta] tokamaks. Here, [ital n] is the toroidal wave number and [beta] is the ratio between plasma and magnetic pressures. The present approach generalizes the standard ballooning-mode formalism and is capable of treating eigenmodes with extended global radial structures, as well as finite coupling between discrete and continuous spectra. Employing the well-known ([ital s],[alpha]) model equilibrium and assuming a linear equilibrium profile, the present approach has been applied to the calculation of the resonant continuum damping rate of TAE modes. Here, [ital s] and [alpha] denote, respectively, the strengths of magnetic shear and pressure gradients. In particular, it is found that there exists a critical [alpha] value, [alpha][sub [ital c]]([ital s]), such that, as [alpha][r arrow][alpha][sub [ital c]], the continuum damping rate is significantly enhanced and, thus, could suppress the potential TAE instability.

OSTI ID:
6022147
Journal Information:
Physics of Fluids B; (United States), Journal Name: Physics of Fluids B; (United States) Vol. 5:10; ISSN 0899-8221; ISSN PFBPEI
Country of Publication:
United States
Language:
English