Table 2.
Simulation parameters. The values of Ma, Md and Ṁd are the same for all simulations.
| # | a | v∞ | v∞/vorb | Ra | Cooling | mg | h̄ | n | |
|---|---|---|---|---|---|---|---|---|---|
| Test models | T1 | 3 | 15 | 0.41 | 20.8 | Adiabatic | 10−10 | 0.24 (0.16–0.40) | 2 × 105 |
| T2 | 3 | 15 | 0.41 | 20.8 | Isothermal | 10−10 | 0.12 (0.01–0.36) | 2 × 105 | |
| T3 | 3 | 15 | 0.41 | 20.8 | Bowen + Schure | 10−10 | 0.13 (0.01–0.37) | 2 × 105 | |
| Test resolution | R1 | 5 | 15 | 0.53 | 34.7 | Bowen + Schure | 10−11 | 0.13 (0.01–0.25) | 3.3 × 106 |
| R2 | 5 | 15 | 0.53 | 34.7 | Bowen + Schure | 4 × 10−11 | 0.20 (0.02–0.39) | 1.1 × 106 | |
| R3 | 5 | 15 | 0.53 | 34.7 | Bowen + Schure | 8 × 10−11 | 0.26 (0.03–0.49) | 5.6 × 105 | |
| Science models | V10a5 | 5 | 10 | 0.35 | 34.7 | Bowen + Schure | 2 × 10−11 | 0.17 (0.06–0.29) | 2.2 × 106 |
| V15a5 | 5 | 15 | 0.53 | 34.7 | Bowen + Schure | 2 × 10−11 | 0.16 (0.01–0.32) | 2.2 × 106 | |
| V30a5 | 5 | 30 | 1.06 | 34.7 | Bowen + Schure | 2 × 10−11 | 0.29 (0.14–0.45) | 2.2 × 106 | |
| V150a5 | 5 | 150 | 5.31 | 34.7 | Bowen + Schure | 2 × 10−11 | 0.50 (0.27–0.78) | 2.2 × 106 | |
| V19a3 | 3 | 19.33 | 0.53 | 20.8 | Bowen + Schure | 2 × 10−11 | 0.07 (0.004–0.22) | 106 | |
| Test sink radius | V10a5s2 | 5 | 10 | 0.35 | 20.8 | Bowen + Schure | 8 × 10−11 | 0.14 (0.01–0.43) | 5.6 × 105 |
| V15a5s2 | 5 | 15 | 0.53 | 20.8 | Bowen + Schure | 2 × 10−11 | 0.08 (0.004–0.28) | 2.2 × 106 | |
| V30a5s2 | 5 | 30 | 1.06 | 20.8 | Bowen + Schure | 2 × 10−11 | 0.28 (0.14–0.45) | 2.2 × 106 |
Notes. The second column corresponds to the name of the model. a is the initial orbital separation of the system in AU. v∞ is the assumed terminal velocity of the wind in km s−1. The ratio v∞/vorb is the ratio of the terminal velocity to the orbital velocity of the system. Ra is the radius of the sink in R⊙. Column 7 specifies the EoS for the model. mg corresponds to the mass of the SPH particles in units of M⊙. h̄ corresponds to the mean smoothing length of the SPH particles within radius a from the centre of mass of the system in units of AU. The numbers in brackets correspond to the 95% confidence interval, i.e. 2.5% of the particles have values below the lower limit and 2.5% particles have values above the upper limit of the given interval. The final column gives the total number of particles n generated at the end of the simulation.
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