1995
DOI: 10.1063/1.871238
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Oscillating field current drive and nonlinear plasma response in bootstrapped tokamaks

Abstract: The nonlinear response of bootstrapped tokamaks to oscillating field current drive (OFCD) is studied with the aid of a formal mathematical solution. The tokamak plasma response to OFCD is shown to be similar to that of a driven inductor–resistor (LR) circuit, but the effective plasma resistance can be negative. A physical picture is constructed in which the tokamak bootstrap effect is viewed as a nonlinear amplification of the plasma magnetic helicity. The bootstrap amplifier can rectify the toroidal plasma cu… Show more

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Cited by 1 publication
(9 citation statements)
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“…where L e is the energy inductance and the volume averaged internal inductance i = B 2 θ /B 2 θa , with B θa the poloidal magnetic field at the plasma edge. For a rigid current profile, we also showed in [2] that the resistance reduction factor ξ bs has the form…”
Section: Magnetic Helicity Modelmentioning
confidence: 68%
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“…where L e is the energy inductance and the volume averaged internal inductance i = B 2 θ /B 2 θa , with B θa the poloidal magnetic field at the plasma edge. For a rigid current profile, we also showed in [2] that the resistance reduction factor ξ bs has the form…”
Section: Magnetic Helicity Modelmentioning
confidence: 68%
“…Finally, we complete our specification of the magnetic helicity model by assuming that the plasma current profile is rigid, as was already mentioned in the introduction. That is, we assume that the circuit elements L h and R nc are fixed [2], dL h /dt = 0 and dR nc /dt = 0. From definitions (35) and (41), the helicity inductance and the neoclassical resistance can then be approximated as…”
Section: Magnetic Helicity Modelmentioning
confidence: 99%
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