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Table 1.

Table of simulations.

Run IC type AB Av N⊥ N∥ Λ η α
1 IEq+Pw 0.02 0.02 64 64 1 5 × 10−6 –
2 IEq+Pw 0.05 0.05 64 64 1 5 × 10−6 –
3 IEq+Pw 0.1 0.1 64 64 1 5 × 10−6 –
4 IEq+Pw 0.2 0.2 64 64 1 5 × 10−6 –
5 IEq+Pw 0.02 0.02 64 64 2 5 × 10−6 –
6 IEq+Pw 0.02 0.02 64 64 3 5 × 10−6 –
7 IEq+Pw 0.02 0.02 64 64 4 5 × 10−6 –
8 IEq+Pw 0.02 0.02 64 64 5 5 × 10−6 –
9 IEq+Pw 0.02 0.02 64 64 6 5 × 10−6 –
10 IEq+Pw 0.02 0.02 64 64 7 5 × 10−6 –
11 IEq+Pw 0.02 0.02 64 64 8 5 × 10−6 –
12 IEq+Pw 0.02 0.02 64 64 9 5 × 10−6 –
13 IEq+Pw 0.02 0.02 64 64 10 5 × 10−6 –
14 HEq+Tb 0.01 0.01 512 16 4 10−8 –
15 IEq+Pw 0.01 0.01 512 16 4 10−8 0.0
16 IEq+Pw+Tb 0.01 0.01 512 16 4 10−8 0.23
17 IEq+Pw+Tb 0.01 0.01 512 16 4 10−8 0.5
18 IEq+Pw+Tb 0.01 0.01 512 16 4 10−8 0.66
19 IEq+Pw+Tb 0.01 0.01 512 16 4 10−8 0.83
20 IEq+Pw+Tb 0.01 0.01 512 16 4 10−8 1.0
21 IEq+Sw 0.01 × 2 $ 0.01 \times \sqrt{2} $ 0.0 512 16 4 10−8 0.0
22 IEq+Sw+Tb 0.01 × 2 $ 0.01 \times \sqrt{2} $ 0.0 512 16 4 10−8 0.23
23 IEq+Sw+Tb 0.01 × 2 $ 0.01 \times \sqrt{2} $ 0.0 512 16 4 10−8 0.5
24 IEq+Sw+Tb 0.01 × 2 $ 0.01\times \sqrt{2} $ 0.0 512 16 4 10−8 0.66
25 IEq+Sw+Tb 0.01 × 2 $ 0.01 \times \sqrt{2} $ 0.0 512 16 4 10−8 0.83
26 IEq+Sw+Tb 0.01 × 2 $ 0.01\times \sqrt{2} $ 0.0 512 16 4 10−8 1.0
27 IEq+Tb 0.005 × 2 $ 0.005 \times \sqrt{2} $ 0.0 512 16 4 10−8 1.0
28 IEq+Tb 0.0023 × 2 $ 0.0023 \times \sqrt{2} $ 0.0 512 16 4 10−8 1.0

Notes. From left to right are reported: a number identifying the Run, the initial perturbation type, the amplitudes AB and Av for the magnetic and the velocity field, respectively, the number of mesh points in the perpendicular and parallel directions, the aspect ratio Λ, the hyper-dissipative coefficient η, and the parameter α, when appropriate. For all the simulations, we used a plasma-β = 5 × 10−2. In the second column, IEq and HEq indicate the inhomogeneous or homogeneous equilibrium, respectively; Pw and Sw indicate the propagating and the standing Alfvén wave, respectively; and Tb indicates the turbulent perturbation. All runs are 3D.

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