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Theory of a high- n toroidicity-induced shear Alfven eigenmode in tokamaks

Journal Article · · Physics of Fluids B; (USA)
DOI:https://doi.org/10.1063/1.859245· OSTI ID:6896532
 [1];  [2]
  1. Center for Fusion Engineering, The University of Texas at Austin, Austin, TX (USA) Institute for Fusion Studies, The University of Texas at Austin, Austin, TX (USA)
  2. Princeton Plasma Physics Laboratory, Princeton University, Princeton, NJ (USA)
A high-{ital n} WKB-ballooning mode equation is employed to study toroidicity-induced shear Alfven eigenmodes (TAE) in {ital s}-{alpha} space, where {ital s}=({ital r}/{ital q})({ital dq}/{ital dr}) is the magnetic shear and {alpha}={minus}(2{ital Rq}{sup 2}/{ital B}{sup 2})({ital dp}/{ital dr}) is the normalized pressure gradient for tokamak plasmas. In the ballooning mode first stability region, TAE modes are found to exist only for {alpha} less than some critical value {alpha}{sub {ital c}}. It is found that these TAE modes reappear in the ballooning mode second stability region for bands of {alpha} values. The global envelope structures of these TAE modes are studied by the Wentzel--Kramers--Brillouin (WKB) method and are found to be bounded radially if the local mode frequency has a maximum in radius.
DOE Contract Number:
AC02-76CH03073; FG05-80ET53088
OSTI ID:
6896532
Journal Information:
Physics of Fluids B; (USA), Journal Name: Physics of Fluids B; (USA) Vol. 2:5; ISSN 0899-8221; ISSN PFBPE
Country of Publication:
United States
Language:
English