Improved model for transport driven by drift modes in tokamaks

A comparison is made between two versions of the Weiland model for computing anomalous transport driven by drift modes such as the ion temperature gradient (ITG) and trapped electron mode (TEM) in tokamak plasmas. Both are quasilinear fluid models that include physical effects resulting from finite Β, magnetic shear, electron-ion collisions, impurities, and fast ions. An outline of the derivation is presented for the newer Weiland19 model, which includes a more accurate description of the effects of finite Β, low and negative magnetic shear, plasma elongation, varying correlation lengths, particle pinch, and momentum transport. It is shown that the two models produce nearly the same ion thermal diffusivity as a function of normalized temperature gradient in a circular plasma with moderate magnetic shear, low Β, and moderately low density gradient. The models differ significantly at low magnetic shear and in elongated plasmas with high Β. In addition, the two models differ significantly in the behavior of the transition between moderate transport driven by ITG/TEM modes at low Β and large transport driven by magnetohydrodynamic instabilities at high Β. In the older Weiland14 model, the transition occurs at a low value of Β that is insensitive to plasma elongation and magnetic shear. In the newer Weiland19 model, the transition occurs at a relatively large value of Β that is a sensitive function of plasma elongation and magnetic shear.