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(Received 12 July 1989; accepted 19 January 1990)
A high-n WKB-ballooning mode equation is employed to study toroidicity-induced shear Alfvén eigenmodes (TAE) in s-
space, where s=(r/q)(dq/dr) is the magnetic shear and
=(2Rq2/B2)(dp/dr) is the normalized pressure gradient for tokamak plasmas. In the ballooning mode first stability region, TAE modes are found to exist only for
less than some critical value
c. It is found that these TAE modes reappear in the ballooning mode second stability region for bands of
values. The global envelope structures of these TAE modes are studied by the WentzelKramersBrillouin (WKB) method and are found to be bounded radially if the local mode frequency has a maximum in radius.
Physics of Fluids B: Plasma Physics is copyrighted by The American Institute of Physics.
DOI: 10.1063/1.859245
PACS:
52.35.Bj, 52.55.Fa
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tokamak plasmas
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