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The mechanism of sawtooth precursors and sawtooth relaxations

Journal Article · · Physics of Fluids B; (USA)
DOI:https://doi.org/10.1063/1.859242· OSTI ID:6999926
; ; ;  [1]
  1. Institut fuer Plasmaphysik der Forschungszentrum, Juelich, GmbH, Juelich (DE) Association EURATOM-KFA, Postfach 1913, 5170 Juelich, Federal Republic of Germany (DE)
It is shown that certain specific properties are requested from the current density profile in order to arrive at a coherent theoretical explanation of the sawtooth phenomenon in tokamaks: (1) the shear {ital {cflx s}} must be small at the {ital q}=1 surface (hence the current density profile has a plateau or shoulder in the neighborhood of {ital q}=1); (2) {ital J}{prime} varies abruptly not far away from {ital q}=1 (in particular, the outer edge of the plateau is close to {ital q}=1). Indeed, when these conditions are satisfied, the contribution to the jump of the derivative of the magnetohydrodynamic (MHD) solution (({Psi}{prime}){sub {ital r}{sub 1}}) from those terms that are proportional to {epsilon}{sup 2} ({epsilon} is the inverse aspect ratio) is not negligible. It is, moreover, opposite in sign to the usual contribution (({Psi}{sup (0){prime}}){sub {ital r}{sub 1}}{proportional to}{ital {cflx s}}{sub 1}) so that the inverse of the logarithmic jump 1/{Delta}{prime}{proportional to}{Psi}{sub {ital r}{sub 1}}/({Psi}{prime}){sub {ital r}{sub 1}} can now take on either positive values ({ital {cflx s}}{sub 1}{gt}{ital {cflx s}}{sub 1,{ital c}}), or negative ones ({ital {cflx s}}{sub 1}{lt}{ital {cflx s}}{sub 1,{ital c}}), or can diverge'' (1/{Delta}{prime}{r arrow}{plus minus}{infinity} for {ital {cflx s}}{sub 1}{r arrow}{ital {cflx s}}{sub 1,{ital c}}).
OSTI ID:
6999926
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