Table 3
Relevant results from the evolutionary calculations that characterise the TP-(S)AGB of our models.
| M ZAMS | Number TP | ⟨ Mcsh ⟩ | ⟨ Mdu ⟩ | ⟨ λ ⟩ | ⟨ THeBS ⟩ | ⟨ THBS ⟩ | ⟨ TBCE ⟩ | ⟨ ΔtIP ⟩ | M core,f | M env,f | |
| M ⊙ | M ⊙ | M ⊙ | MK | MK | MK | yr | M ⊙ | M ⊙ | |||
|
|
|||||||||||
| 4.0 | 197 | 3.6 × 10-3 | 2.7 × 10-3 | 0.92 | 359.1 | 90.5 | 84.7 | 6702 | 0.93 | 0.25 | |
| 5.0 | 213 | 2.6 × 10-3 | 1.9 × 10-3 | 0.91 | 356.7 | 95.1 | 88.4 | 4382 | 0.97 | 0.54 | |
| 6.0 | 372 | 1.4 × 10-3 | 9.8 × 10-4 | 0.85 | 361.8 | 104.1 | 98.7 | 1828 | 1.04 | 0.69 | |
| 7.0 | 607 | 5.8 × 10-4 | 3.9 × 10-4 | 0.78 | 366.8 | 116.5 | 113.6 | 739 | 1.14 | 0.73 | |
| 8.0 | 1114 | 1.6 × 10-4 | 6.2 × 10-5 | 0.48 | 363.1 | 130.8 | 127.6 | 183 | 1.26 | 0.53 | |
| 9.0 | 1138 | 2.3 × 10-5 | 1.1 × 10-5 | 0.05 | 362.4 | 147.5 | 144.7 | 30 | 1.35 | 1.52 | |
Notes. Angled brackets indicate linear averages over the total number of pulses. From left to right we give: the initial mass, the number of computed thermal pulses, the mass of the intershell convective region, the amount of material dredged-up after each pulse, the dredge-up parameter, the maximum temperature reached in the inner convective region at each pulse, the maximum temperatures at the base of the H-shell (defined as the point at which H-mass fractions ≲0.05) and at the base of the convective envelope at each interpulse, the interpulse period (defined as the time between two consecutive pulses p + 1 and p) and the final core and envelope masses at the end of our calculations.
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