2015
DOI: 10.1063/1.4914841
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Flux-driven simulations of turbulence collapse

Abstract: Using three-dimensional nonlinear simulations of tokamak turbulence, we show that an edge transport barrier (ETB) forms naturally once input power exceeds a threshold value. Profiles, turbulence-driven flows, and neoclassical coefficients are evolved self-consistently. A slow power ramp-up simulation shows that ETB transition is triggered by the turbulence-driven flows via an intermediate phase which involves coherent oscillation of turbulence intensity and E Â B flow shear. A novel observation of the evolutio… Show more

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Cited by 33 publications
(39 citation statements)
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“…1,2 Efforts to understand the low (L) mode to high (H) mode confinement transition in tokamaks have further increased interest in this topic. [3][4][5][6][7][8][9][10][11] A closely related subject is that of understanding the saturation mechanism for edge and SOL turbulence. 12,13 In addition to contributing to L-H mode transition physics, some models predict that turbulence in the vicinity of the separatrix could be sufficiently large so as to impact the width of the heat flux channel.…”
Section: Introductionmentioning
confidence: 99%
“…1,2 Efforts to understand the low (L) mode to high (H) mode confinement transition in tokamaks have further increased interest in this topic. [3][4][5][6][7][8][9][10][11] A closely related subject is that of understanding the saturation mechanism for edge and SOL turbulence. 12,13 In addition to contributing to L-H mode transition physics, some models predict that turbulence in the vicinity of the separatrix could be sufficiently large so as to impact the width of the heat flux channel.…”
Section: Introductionmentioning
confidence: 99%
“…The transfer of energy between fluctuations and sheared flows has also been demonstrated by fluid simulations for interchange turbulence with cold ions [10][11][12]. Recently, the formation of transport barrier has been simulated with fluid models [17][18][19], in which the neoclassical terms are added in the vorticity equation with cold ions. In these simulations [17][18][19], the mean shear flows are generated mainly due to the neoclassical terms.…”
Section: Introductionmentioning
confidence: 99%
“…where represents the contribution of ion diamagnetic drift to the polarization current [3,4,[6][7][8], which is the crucial difference from the cold ion model [9][10][11][12][13][14][15][16][17][18][19]. The source terms S n and S E are added in Eqs.…”
Section: Model Equationsmentioning
confidence: 99%
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