Dynamics of Shear Layer Collapse in Modified Hasegawa--Wakatani Channel Flows

Density limit phenomenology has been associated with the collapse of edge shear layers at high density. Theoretical work has suggested that the onset of such collapse occurs when adiabaticity $\alpha=k_{\parallel}^{2}V_{th}^{2}/\omega\nu$ drops below $\alpha_{crit}\approx1$. Here, we explored shear flow dynamics in a spatially varying $\alpha\left(x\right)$ profile. $\alpha<\alpha_{crit}$ on the outer boundary, and $\alpha>\alpha_{crit}$ on the inner one. The gradient in $\alpha$ triggers the formation of a barrier shear layer, which separates the regions of isotropic turbulence and zonal flows. The barrier is pinned to the location of $\alpha_{crit}$ and does not propagate. Work on the effect of a spatially profiled neutral drag (reflecting a neutral profile) is ongoing. More generally, we report on some interesting differences between zonal flow phenomena in the conventional doubly periodic box and in channel flows. Specifically: i) Zonal flows are more coherent in the channel flow. ii) A transition curve of $R=\frac{ZF Energy}{Total Kinetic Energy}$ is largely monotonic in for the box. More complex behavior is shown in the case of the channel flow. iii) Time histories are different for the box and channel cases. Work on all the issues discussed above is ongoing.