Table 1
Parameters of the models studied.
| Model | rinit (AU) | tout (yr) | rsep (AU) | rv=0 at tout (AU) | Linit (L⊙) | Lout (L⊙) | α |
|---|---|---|---|---|---|---|---|
| Nominal | 20 | – | 6.90 at t = 1 kyr | 2.88 at t = 1 kyr | 1 | 10−2 | |
| Compact | 2.5 | – | 7.54 at t = 1 kyr | 1.62 at t = 1 kyr | 1 | 10−2 | |
| Outburst | 20 | 104 | 67.15 at tout | 15.91 at tout | 1 | 1000 | 10−2 |
| Outburst-NoVisc | 20 | 104 | 67.15 at tout | 12.53 at tout | 1 | 1000 | 10−2 |
| Med-Outburst | 20 | 104 | 42.32 at tout | 12.52 at tout | 1 | 500 | 10−2 |
| Small-Outburst | 20 | 104 | 14.57 at tout | 12.52 at tout | 1 | 100 | 10−2 |
| Late-Outburst | 20 | 105 | 67.15 at tout | 17.42 at tout | 1 | 1000 | 10−2 |
| Med-visc-alpha | 20 | 104 | 67.15 at tout | 12.26 at tout | 1 | 1000 | 5×10−2 |
| Low-visc-alpha | 20 | 104 | 67.15 at tout | 12.03 at tout | 1 | 1000 | 10−3 |
Notes. The value of tout corresponds to the time when the outburst is introduced in the outburst models. The parameter rsep describes the radial distance where the processed and unprocessed components are separated. The radius rv=0 indicates the initial distance where the gas advection changes direction from moving toward the star to expanding outward viscously to conserve angular momentum.
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