Nuclear Fusion · 2016 · 33 citations · 38 references
Natural SciencesPhysicsFusion EngineeringNuclear PhysicsPlasma PhysicsDivertor EngineeringPlasma ConfinementDivertor PhysicsLangmuir ProbesParticle Flux DynamicsParticle Flux MeasurementTokamak PhysicsToroidal ConfinementX-point Divertors
Abstract The in–out divertor asymmetry in the Experimental Advanced Superconducting Tokamak (EAST), as manifested by particle fluxes measured by the divertor triple Langmuir probe arrays, is significantly enhanced during type-I edge localized modes (ELMs), favoring the inner divertor in lower single null (LSN) for the normal toroidal field ( B t ) direction, i.e. with the ion B × <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mstyle displaystyle="false"> <mml:mo>∇</mml:mo> </mml:mstyle> </mml:math> B direction towards the lower X -point, while the in–out asymmetry is reversed when the ion B × <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mstyle displaystyle="false"> <mml:mo>∇</mml:mo> </mml:mstyle> </mml:math> B is directed away from the lower X -point. The plasma flow measured by the Mach probe at the outer midplane is in the ion Pfirsch–Schlüter (PS) flow direction, opposite to both B × <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mstyle displaystyle="false"> <mml:mo>∇</mml:mo> </mml:mstyle> </mml:math> B and E × B drifts, i.e. towards the inner divertor for normal B t , and the outer divertor for reverse B t , consistent with the observed in–out divertor asymmetry in particle fluxes. Since the particle source from an ELM event is predominantly located near the outer midplane, this new finding suggests a critical role of the PS flow in driving the in–out divertor asymmetry. The divertor asymmetry during type-III ELMs exhibits a similar trend to that during type-I ELMs. Strong in–out divertor asymmetry is also present during inter-ELM and ELM-free phases for the normal field direction, i.e. with more particle flux to the lower inner divertor target, but the peak particle flux merely becomes more symmetric, or slightly reversed, for reverse B t , i.e. reversed B × <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mstyle displaystyle="false"> <mml:mo>∇</mml:mo> </mml:mstyle> </mml:math> B drift direction.
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A long-pulse high-confinement plasma regime in the Experimental Advanced Superconducting Tokamak
J. Li, Huan Guo, Baonian Wan et al. · Nature Physics · 2013 · 292 citations