Table 2
Properties of inhomogeneous cloud simulations.
| Name | N c | n | lc/ Λc | τ p / τ c | N s | ι | τ | φ |
|
|
||||||||
| C1 | 10 | 36 | 3 | 3 | 3 | 0.2 | 0.7 | 0.1 |
| C2 | 10 | 36 | 1 | 1 | 2 | 0.5 | 0.9 | 0.2 |
| C3 | 50 | 22 | 4 | 7 | 0 | 0.1 | 0.2 | 0.1 |
| C4 | 50 | 23 | 2 | 3 | 1 | 0.2 | 0.3 | 0.1 |
| C5 | 100 | 28 | 5 | 10 | 1 | 0.6 | 0.3 | 0.03 |
| C6 | 10 | 330 | 1 | 1 | 5 | 0.2 | 0.7 | 0.1 |
| C7 | 10 | 330 | 1 | 1 | 14 | 0.4 | 0.9 | 0.2 |
| C8 | 3 | 570 | 2 | 1 | 9 | 0.2 | 0.6 | 0.1 |
| C9 | 3 | 570 | 1 | 1 | 8 | 0.7 | 0.7 | 0.3 |
| C10 | 10 | 330 | 5 | 9 | 5 | 0.04 | 0.8 | 0.02 |
| C11 | 20 | 261 | 12 | 13 | 5 | 0.04 | 0.7 | 0.02 |
| C12 | 20 | 261 | 12 | 35 | 9 | 0.01 | 0.8 | 0.06 |
| C13 | 40 | 208 | 4 | 6 | 2 | 0.2 | 0.5 | 0.1 |
| C14 | 40 | 208 | 12 | 33 | 3 | 0.03 | 0.6 | 0.01 |
| C15 | 40 | 208 | 2 | 2 | 7 | 0.4 | 0.5 | 0.2 |
| C16 | 5 | 159 | 2 | 2 | 8 | 0.2 | 0.9 | 0.1 |
| C17 | 5 | 159 | 6 | 11 | 3 | 0.03 | 0.9 | 0.01 |
| C18 | 5 | 159 | 1 | 1 | 6 | 0.7 | 0.9 | 0.3 |
| C19 | 10 | 180 | 8 | 16 | 6 | 0.2 | 0.3 | 0.1 |
| C20 | 10 | 181 | 3 | 3 | 8 | 0.1 | 0.3 | 0.07 |
| C21 | 10 | 181 | 1 | 1 | 9 | 0.3 | 0.3 | 0.1 |
| C22 | 20 | 181 | 3 | 4 | 4 | 0.1 | 0.3 | 0.06 |
| C23 | 20 | 186 | 2 | 2 | 3 | 0.3 | 0.6 | 0.2 |
Notes. The columns are: Nc number of centres, n = N/ 103 where N is the total number of particles, lc/ Λc ratio between the size of a subcloud and the average distance between centres, τp/τc ratio between the time of collapse of a subcloud and that of the cloud, Ns is the number of satellite after the collapse and ι,τ, φ are the shape parameters of the initial conditions.
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