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Enhanced performance in quasi-isodynamic max-$J$ stellarators with a turbulent particle pinch

G. G. Plunk, A. G. Goodman, P. Xanthopoulos, P. Costello, H. M. Smith, K. Aleynikova, C. D. Beidler, M. Drevlak, P. Helander

Abstract

Recent stellarator reactor designs demonstrate mostly outward turbulent particle transport, which, without advanced fueling technology, inhibits the formation of density gradients needed for confinement. We introduce ``SQuID-$τ$'', a self-fueling quasi-isodynamic stellarator capable of sustaining density peaking through inward particle transport caused by turbulence. Temperature and density profile predictions based on high-fidelity gyrokinetic simulations demonstrate enhanced performance, significantly relaxing constraints on the size and magnetic field strength for reactor designs.

Enhanced performance in quasi-isodynamic max-$J$ stellarators with a turbulent particle pinch

Abstract

Recent stellarator reactor designs demonstrate mostly outward turbulent particle transport, which, without advanced fueling technology, inhibits the formation of density gradients needed for confinement. We introduce ``SQuID-'', a self-fueling quasi-isodynamic stellarator capable of sustaining density peaking through inward particle transport caused by turbulence. Temperature and density profile predictions based on high-fidelity gyrokinetic simulations demonstrate enhanced performance, significantly relaxing constraints on the size and magnetic field strength for reactor designs.

Paper Structure

This paper contains 4 equations, 4 figures.

Figures (4)

  • Figure 1: The self-fueling quasi-isodynamic stellarator design SQuID-$\tau$, shown with its filamentary coil set.
  • Figure 2: Total heat fluxes from GX simulations for Stellaris (top; dashed) and SQuID-$\tau$ (bottom; dashed), compared with those of W7-X standard configuration (solid) for $\eta(\rho) = \eta_\mathrm{exp}$ and $\eta(\rho) = \eta_\mathrm{crit}$, respectively. Note that data appears in order of increasing $s = \sqrt{\psi/\psi_\mathrm{edge}}$, from left to right in the figures.
  • Figure 3: Experimental profiles (fitted) of reference scenarios, compared against theoretical profiles, including (solid) and excluding (dashed) neoclassical contribution to heat flux. The edge/core boundary conditions for theoretical temperature profiles are set to the experimental values.
  • Figure 4: Accessible design points for a stellarator reactor with fusion gain $Q = 1$.