W7-X EM turbulence

Motivation

  1. Flux tubes are not equivalent (in contrast to tokamaks): stellarators are intrinsically poloidally-global.
  2. Radial bounce-averaged drifts do no vanish (in contrast to tokamaks): stellarators are intrinsically radially-global.
  3. No good way to incorporate ambient Er in a flux tube.

Geometry and profiles

Larger temperature implies larger ρ (relevant values Te5[keV])
Larger ρ need less Fourier harmonics to resolve the same kρi1

Time evolution (β=1.12%)


Heat and particle fluxes in gyro-Bohm units; profile evolution is not strong


Initialization with noise; instability starts to develop


Linear instability; ZF is excited; linear mode is weaken locally by ZF


The turbulence is pushed by ZF into regions of small gradient; saturation

Beta scan: electrostatic potential

on the left: zonal flow included. On the right: zonal flow excluded

Summary: zonal flow excited at larger β is weaker

Evolution of electrostatic potential (β=1.12%) plotted as a function of radius and toroidal mode number; including zonal flow and temperature evolution

Evolution of electrostatic potential (β=1.12%) plotted as a function of radius and toroidal mode number; excluding zonal flow
Evolution of electrostatic potential (β=1.12%) plotted in a poloidal cross-section; all modes included