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Table 1.
Parameters, grid spacing and radial extension of the simulations discussed in the paper.
| Name | βini | ϵ | r domain | φ domain | Resolution | t1 | t2 = Tend |
|---|---|---|---|---|---|---|---|
| SB4 | 104 | 0.1 | [1, 200] | [ − π/4, π/4] | [850,176L+64S,62] | 923Tin | 1114Tin |
| SB3 | 103 | 0.1 | [1, 200] | [ − π/4, π/4] | [850,176L+64S,62] | 923Tin | 1114Tin |
| SB2 | 102 | 0.1 | [1, 200] | [ − π/4, π/4] | [850,176L+64S,62] | 1719Tin | 1910Tin |
| SEp | 104 | 0.05 | [1, 100] | [ − π/4, π/4] | [1475, 96L+70S+2L, 62] | 923Tin | 1114Tin |
| S2pi | 104 | 0.1 | [1, 200] | [0, 2π] | [850,176L+64S,256] | 923Tin | 1034Tin |
Notes. The latitudinal grid is not homogeneous, with grid spacing varing linearly (L) close to the disk and geometrically (S = stretched) close to the poles. We define Tin = TK(Rin) where TK(R) = 2π/ΩK(R).
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