4.5 Article

Achieving a robust grassy-ELM operation regime in CFETR

Journal

NUCLEAR FUSION
Volume 60, Issue 4, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/1741-4326/ab72c0

Keywords

grassy-ELMs; collisionality; high beta(p); peeling-ballooning mode; CFETR; experimental comparison

Funding

  1. National Magnetic Confinement Fusion Program of China [2017YFE0300500, 2017YFE0300501, 2015GB111001]

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We have identified a robust grassy-edge localized mode (ELM) operation regime for future tokamak reactors. The regime exists within a pedestal top electron collisionality (nu*) window at high global poloidal beta (beta(p)). The existence of an upper nu* limit for grassy-ELMs is consistent with results previously reported in experiments (Oyama et al 2010 Nucl. Fusion 50 064014), while the existence of a lower nu* limit has not been reported previously. Using EPED and BOUT + +, a theoretical model that quantitatively explains the physics of the grassy-ELMs within the window, which distinguishes them from the small mixed-ELMs at lower nu*, is presented for the first time. A peeling-ballooning stability boundary is obtained by scanning the operating density space. The change in density corresponds to a change in nu* that affects the pedestal bootstrap current. High beta(p) leads to a strong Shafranov shift, which affects the flux surface averaged pressure drive. The two effects combine to create a peeling-dominated window in intermediate nu* buffered by ballooning-dominated regimes. Only the peeling-dominated regime shows a cyclic behavior in the perturbed pressure during the nonlinear simulation of an ELM crash, reminiscent of grassy-ELM dynamics. Similarly, the energy released across the separatrix is demonstrated to be significantly smaller. The quick recovery of the ELM crash is explainable by the rapid rise of a low n kink-peeling instability when the pedestal current I-ped exceeds a threshold at high beta(p). It minimizes the excursion beyond marginal stability and is absent in the ballooning-dominated regime. Comparison with recent experiments over a range of beta(p) and nu* strongly supports the physical picture proposed by the modeling.

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