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Table 1:

Overview and results of all the simulations.

Model
$\rho_{\rm g}$ $\alpha$ $r_{\rm m}$ $\max (\bar{m})$ $\max (\bar{\Psi})$ $\Psi _{\rm min}$ $t_{{\rm noc}}$ $\max(\bar{St})$
  [g cm-3]     [g]     [yr]  
(1) (2) (3) (4) (5) (6) (7) (8) (9)

Lt1d-3m100
$2.4 \times 10^{-11}$ 10-3 100 $8\times 10^{-8}$ 7.27 1.77 $2\times 10^{4}$ $2.5\times 10^{-4}$
Lt1d-4m100 $2.4 \times 10^{-11}$ 10-4 100 $9.7 \times 10^{-8}$ 7.12 2.23 $8\times 10^{4}$ $2.2 \times 10^{-4}$
Lt1d-5m100 $2.4 \times 10^{-11}$ 10-5 100 $2.66 \times 10^{-7}$ 7.72 3.78 $3 \times 10^{5}$ $2.1 \times 10^{-4}$
Mt1d-3m100 $1.4 \times 10^{-9}$ 10-3 100 8.13 24.41 3.88 104 $5.1\times 10^{-4}$
Mt1d-4m100 $1.4 \times 10^{-9}$ 10-4 100 4.18 21.9 1.85 $2\times 10^5$ $2.8 \times 10^{-4}$
Mt1d-5m100 $1.4 \times 10^{-9}$ 10-5 100 $7.7\times 10^{-2}$ 30.0 4.13 $7\times 10^{5}$ $2.1 \times 10^{-4}$
Ht1d-3m100 $2.7\times 10^{-8}$ 10-3 100 3.77 34.1 5.61 105 $1.4 \times 10^{4}$
Ht1d-4m100 $2.7\times 10^{-8}$ 10-4 100 0.23 38.0 5.41 $3\times 10^6$ $3.6 \times 10^{-5}$
Ht1d-5m100 $2.7\times 10^{-8}$ 10-5 100 0.28 43.9 4.94 $4\times 10^6$ $7.7\times 10^{-5}$
Lt1d-4m10 $2.4 \times 10^{-11}$ 10-4 10 $9.2\times 10^{-4}$ 5.88 2.28 105 $3.8 \times 10^{-3}$
Lt1d-4m100 $2.4 \times 10^{-11}$ 10-4 100 $9.7 \times 10^{-8}$ 7.12 2.23 $8\times 10^{4}$ $2.2 \times 10^{-4}$
Lt1d-4m1000 $2.4 \times 10^{-11}$ 10-4 1000 $9.7 \times 10^{-8}$ 7.09 2.29 $8\times 10^{4}$ $2.2 \times 10^{-4}$
Mt1d-4m10 $1.4 \times 10^{-9}$ 10-4 10 $2.5\times 10^{-2}$ 19.4 2.1 $2\times 10^5$ $2.2 \times 10^{-4}$
Mt1d-4m100 $1.4 \times 10^{-9}$ 10-4 100 4.18 21.9 1.85 $2\times 10^5$ $2.8 \times 10^{-4}$
Mt1d-4m1000 $1.4 \times 10^{-9}$ 10-4 1000 $9.5 \times 10^{-3}$ 23.1 2.9 $2\times 10^5$ $1.3\times 10^{-4}$
Ht1d-4m10 $2.7\times 10^{-8}$ 10-4 10 0.15 34.6 2.46 $2\times 10^6$ $4.5\times 10^{-5}$
Ht1d-4m100 $2.7\times 10^{-8}$ 10-4 100 0.23 38.0 5.41 $3\times 10^6$ $3.6 \times 10^{-5}$
Ht1d-4m1000 $2.7\times 10^{-8}$ 10-4 1000 $8.8 \times 10^{-2}$ 40.0 7.1 105 $3.5\times 10^{-5}$

Notes. In this table, Col. 1 describes the model names. ``L'' stands for the low density model, ``M'' is the MMSN model, ``H'' is the high density model, the letter ``t'' and the following number indicates the value of the turbulence parameter, the letter ``m'' and the number shows the used critical mass ratio values. Columns 2-4 shows the gas density, turbulence parameter, and the critical mass ratio respectively. Columns 5-9 list the parameters defined to characterize the distribution functions. These are the average maximum mass in Col. 5, the average maximum enlargement parameter in Col. 6, the minimum enlargement parameter in Col. 7, the end of the compaction phase in Col. 8, and the average maximum Stokes number in Col. 9.


Source LaTeX | All tables | In the text

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