Table 4
Simulations with ambipolar diffusion.
| Name | 104B0 |
|
ℒ |
|
State |
|
|
|||||
| A3N0 | 10 | 25(0.1) | 1 | 1.0 × 10-3 | 2 bands |
| A3N1 | 10 | 25(0.1) | 2 | 1.1 × 10-3 | 3 bands |
| A3N2 | 10 | 2.5(0.01) | 1 | 7.3 × 10-4 | 2 bands |
| A3N3 | 10 | 2.5(0.01) | 0.4 | 9.6 × 10-4 | 2 bands |
| A3N4 | 10 | 2.5(0.01) | 0.2 | 1.5 × 10-3 | 2 bands |
| A4N5 | 1 | 25(0.01) | 1 | 1.3 × 10-3 | channel |
| A4N6 | 1 | 25(0.01) | 4 | 1.1 × 10-3 | 3 bands |
| ABS | 18 | 139Ω(1) | 0 | 4.2 × 10-3 | turbulent |
Notes. Parameters for the 3D Hall+Ambipolar MHD runs. Columns: label of the run, mean vertical magnetic field B0; ambipolar Lundquist number 
; corresponding ambipolar Elsasser number 
at the inner radius r0 = 1; Hall parameters ℒ; total turbulent stress ; and final state of the flow. “Channel” describes a computational domain filled with linear HSI modes. Only run ABS has a diffusivity scaling as r3 / 2, corresponding to a constant ambipolar Elsasser number ΛA = 1.
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.