Table 3
Summary of the 20 short-term simulations.
| Sij | V | M | μ | req (m) | ES1 | ES2 | ES3 | ES4 |
|---|---|---|---|---|---|---|---|---|
| S14 | V1 | M4 | 0.90 | 381 | No | No | No | No |
| S13 | V1 | M3 | 0.92 | 381 | No | No | No | No |
| S12 | V1 | M2 | 0.94 | 381 | No | No | No | No |
| S24 | V2 | M4 | 0.95 | 388 | No | No | No | No |
| S11 | V1 | M1 | 0.96 | 381 | Yes | No | No | Yes |
| S23 | V2 | M3 | 0.97 | 388 | Yes | No | No | Yes |
| S22 | V2 | M2 | 0.99 | 388 | Yes | No | No | Yes |
| S34 | V3 | M4 | 1.00 | 395 | Yes | No | No | Yes |
| S21 | V2 | M1 | 1.01 | 388 | Yes | No | No | Yes |
| S33 | V3 | M3 | 1.02 | 395 | Yes | No | No | Yes |
| S32 | V3 | M2 | 1.05 | 395 | Yes | Yes | No | Yes |
| S44 | V4 | M4 | 1.05 | 402 | Yes | Yes | No | Yes |
| S31 | V3 | M1 | 1.07 | 395 | Yes | Yes | Yes | Yes |
| S43 | V4 | M3 | 1.08 | 402 | Yes | Yes | Yes | Yes |
| S42 | V4 | M2 | 1.10 | 402 | Yes | Yes | Yes | Yes |
| S54 | V5 | M4 | 1.10 | 408 | Yes | Yes | Yes | Yes |
| S41 | V4 | M1 | 1.12 | 402 | Yes | Yes | Yes | Yes |
| S53 | V5 | M3 | 1.13 | 408 | Yes | Yes | Yes | Yes |
| S52 | V5 | M2 | 1.15 | 408 | Yes | Yes | Yes | Yes |
| S51 | V5 | M1 | 1.18 | 408 | Yes | Yes | Yes | Yes |
Notes. The subscript i refers to the volume Vi, and j refers to the mass Mj of the Sij simulation. We include the corresponding stability parameter, μ, and the average equatorial radius of the shape model used in the simulation, req. The table is sorted according to increasing values of the stability parameter, μ. The last four columns are a summary of short-term simulations, indicating whether (yes) or not (no) particles were present in each end state at the end of the simulation time. Below the horizontal line, particles may collide with the secondary.
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