Parameters used for N-body runs. In all cases the initial conditions were realizations of the Plummer model (Plummer 1911). The values of trh,i (the initial half-mass relaxation time) are calculated using Λ = 0.02N for the Coulomb logarithm.
| N . | m2/m1 . | M2/M1 . | trh,i (N-body units) . |
|---|---|---|---|
| 32k | 10, 20 | 0.01, 0.02 | 471 |
| 64k | 10, 20 | 0.01, 0.02 | 851 |
| 128k | 20 | 0.02 | 1552 |
| N . | m2/m1 . | M2/M1 . | trh,i (N-body units) . |
|---|---|---|---|
| 32k | 10, 20 | 0.01, 0.02 | 471 |
| 64k | 10, 20 | 0.01, 0.02 | 851 |
| 128k | 20 | 0.02 | 1552 |
Parameters used for N-body runs. In all cases the initial conditions were realizations of the Plummer model (Plummer 1911). The values of trh,i (the initial half-mass relaxation time) are calculated using Λ = 0.02N for the Coulomb logarithm.
| N . | m2/m1 . | M2/M1 . | trh,i (N-body units) . |
|---|---|---|---|
| 32k | 10, 20 | 0.01, 0.02 | 471 |
| 64k | 10, 20 | 0.01, 0.02 | 851 |
| 128k | 20 | 0.02 | 1552 |
| N . | m2/m1 . | M2/M1 . | trh,i (N-body units) . |
|---|---|---|---|
| 32k | 10, 20 | 0.01, 0.02 | 471 |
| 64k | 10, 20 | 0.01, 0.02 | 851 |
| 128k | 20 | 0.02 | 1552 |
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