Progress in extending high poloidal beta scenarios on DIII-D towards a steady-state fusion reactor and impact of energetic particles. (23rd September 2020)

• Record Type: Journal Article
• Authors: Huang, J.; Garofalo, A.M.; Qian, J.P.; Gong, X.Z.; Ding, S.Y.; Varela, J.; Chen, J.L.; Guo, W.F.; Li, K.; Wu, M.Q.; Pan, C.K.; Ren, Q.; Zhang, B.; Lao, L.L.; Holcomb, C.T.; McClenaghan, J.; Weisberg, D.; Chan, V.; Hyatt, A.; Hu, W.H.; Li, G.Q.; Ferron, J.; McKee, G.; Pinsker, R.I.; Rhodes, T.; Staebler, G.M.; Spong, D.; Yan, Z.
• Is Part Of: Nuclear fusion. Volume 60:Number 12(2020)
• Publication Date: 2020-09-23
• Subjects: tokamak -- steady state -- high bootstrap current -- energetic particle; Nuclear fusion -- Periodicals; 621.48405
• DOI: 10.1088/1741-4326/abaf33
• Languages: English
• ISSNs: 0029-5515

Abstract

Abstract: To prepare for steady-state operation of future fusion reactors (e.g. the International Thermonuclear Experimental Reactor and China Fusion Engineering Test Reactor (CFETR)), experiments on DIII-D have extended the high poloidal beta ( β P ) scenario to reactor-relevant edge safety factor q 95 ∼ 6.0, while maintaining a large-radius internal transport barrier (ITB) using negative magnetic shear. Excellent energy confinement quality ( H 98y2 > 1.5) is sustained at high normalized beta ( β N ∼ 3.5). This high-performance ITB state with Greenwald density fraction near 100% and q min ≥ 3 is achieved with toroidal plasma rotation V tor ∼ 0 at ρ ≥ 0.6. This is a key result for reactors expected to have low V tor . At high β P (≥1.9), large Shafranov shift can stabilize turbulence leading to a high confinement state with a low pedestal and an ITB. At lower β P (<1.9), negative magnetic shear in the plasma core contributes to turbulence suppression and can compensate for reduced Shafranov shift to continue to access a large-radius ITB and excellent confinement with low V tor, consistent with the results of gyrofluid transport simulations. These high- β P cases are characterized by weak/no Alfvén eigenmodes (a.e.) and classical fast-ion transport. At high density, the fast-ion deceleration time decreases and Δ β fast is lower; these reduce a.e. drive. The reverse-shear Alfvén eigenmodes are weaker or stable because the negative magnetic shear region is located at higher radius, away from the peaked fast-ion profile. Resistive wall modes can be a limitation at simultaneous high β N, low internal inductance, and low rotation. Analysis suggests that additional off-axis external current drive could provide a more stable path at reduced q 95 . Based on a DIII-D high- β P plasma with large-radius ITB, two scenarios are proposed for CFETR Q = 5 steady-state operation with ∼1 GW fusion power: a lower- l i ( l i ∼ 0.66) and a higher- l i ( l i ∼ 0.75) case. Using a Landau closure model, multiple energetic particle (EP) effects on the a.e. stability are analyzed modifying the growth rate of the a.e.s triggered by the neutral-beam-injection EPs and alpha particles, although the stabilizing/destabilizing effect is weak for the cases analyzed. The stabilizing effects of the combined EP species β, energy, and density profile in CFETR need further investigation.