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Table 1

Summary of the different simulations.

Model Res. Lbox (H) β Am Λ λc,th/H 〈Γo 〈ΓA
O10A10 1283 1 750 10 10 0.18 1.3(−1) 4.8(−9) 8.7(−7) 1.2(−8) 2.8(−6)
O10A10−HR 2563 1 750 10 10 0.18 9(−2) 3.5(−9) 2.9(−7) 7(−9) 7.3(−7)
O10A10−LARGE 2563 2 750 10 10 0.18 3.7(−2) 1.5(−9) 1.2(−7) 3.5(−9) 3.1(−7)
O10A10BETA7500 1283 1 7500 10 10 0.1 3(−3) 5.4(−11) 4.4(−8) 7.9(−11) 1.0(−8)
O1A1 1283 1 750 1 1 0.26 2.5(−2) 3.2(−9) 8.6(−8) 4.8(−9) 1.6(−7)
O10A1 1283 1 750 1 10 0.26 1(−1) 2.5(−9) 2.8(−6) 5.4(−9) 7.7(−6)
O1A10 1283 1 750 10 1 0.18 1.6(−2) 2.1(−9) 3.2(−9) 2.7(−9) 6.4(−9)

Notes. All of them are computed for 50 Ω−1, except for O10A10-HRES, which is only computed 26 Ω−1 for numerical cost reasons and O10A10BETA7500, which is computed for 200 Ω−1, as it takes a longer time to reach a steady state. Res. stands for resolution. is averaged over 10 Ω−1 at the end of the simulation. Dimensional quantities are given in cgs units. We note that the models all have the same Stokes numbers for the 3 grain sizes St = (4 × 10−4, 4 × 10−3, 4 × 10−2).

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