Table 3
Stellar mass, the mass of H, the evolutionary timescale, the radial order and harmonic degree, the Teff-range of instability, the average period, the maximum e-folding time, and the ratio of the evolutionary timescale to the maximum e-folding time, corresponding to unstable short-period ℓ = 1,2g modes for which the ε mechanism strongly contributes to their destabilization, corresponding to model sequences with M⋆ ≤ 0.2389 M⊙ computed using the ML2 prescription of the MLT theory of convection.
M⋆/M⊙ | MH/M⋆ [10-3] | τ [109 yr] | k (ℓ) | Teff[K] | ⟨ Π ⟩[s] |
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0.1554 | 25.4 | 3.13 | 2 (1) | ≲ 8500 | 350 | 0.07 | 44.7 |
3 (1) | 9000−8300 | 470 | 0.97 | 3.2 | |||
2 (2) | ≲ 8100 | 227 | 0.12 | 26.1 | |||
3 (2) | 8600−8360 | 291 | 0.20 | 15.7 | |||
4 (2) | 9000−8800 | 355 | 0.33 | 9.5 | |||
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0.1612 | 20.6 | 4.44 | 2 (1) | ≲ 8950 | 343 | 0.80 | 5.6 |
3 (1) | ≲ 9260 | 448 | 0.44 | 10.1 | |||
1 (2) | ≲ 7150 | 148 | 0.03 | 148.0 | |||
2 (2) | ≲ 8600 | 220 | 0.80 | 5.6 | |||
3 (2) | ≲ 9250 | 283 | 0.60 | 7.4 | |||
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0.1650 | 18.7 | 5.53 | 1 (1) | ≲ 8200 | 250 | 0.07 | 79.0 |
2 (1) | ≲ 9500 | 340 | 0.17 | 32.5 | |||
3 (1) | 9500−9020 | 450 | 1.30 | 4.25 | |||
4 (1) | ≲ 7800 | 580 | 0.80 | 6.9 | |||
2 (2) | ≲ 8950 | 214 | 0.50 | 11.1 | |||
3 (2) | 9400−9300 | 277 | 0.50 | 11.1 | |||
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0.1706 | 16.3 | 6.59 | 1 (1) | 9660−9600 | 255 | 0.05 | 131.8 |
2 (1) | ≲ 9979 | 350 | 1.05 | 6.3 | |||
3 (1) | ≲ 7750 | 480 | 2.50 | 2.6 | |||
1 (2) | ≲ 9060 | 151 | 0.01 | 659 | |||
2 (2) | ≲ 9650 | 223 | 1.95 | 3.4 | |||
3 (2) | 7730−7180 | 310 | 0.58 | 11.4 | |||
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0.1762 | 14.5 | 7.56 | 1 (1) | ≲ 9100 | 247 | 1.40 | 5.4 |
2 (1) | ≲ 10 000 | 320 | 0.20 | 37.8 | |||
3 (1) | ≲ 8700 | 470 | 0.70 | 10.8 | |||
4 (1) | 8900−8700 | 550 | 0.09 | 84 | |||
5 (1) | 9200−9150 | 620 | 0.06 | 126 | |||
1 (2) | ≲ 8300 | 140 | 0.02 | 378 | |||
2 (2) | ≲ 9900 | 220 | 0.40 | 18.9 | |||
3 (2) | 8300−7700 | 297 | 0.25 | 30.4 | |||
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0.1806 | 3.68 | 0.34 | 1 (1) | ≲ 10 500 | 270 | 0.05 | 6.8 |
2 (1) | 10 200−9700 | 355 | 0.02 | 17 | |||
1 (2) | ≲ 10 500 | 178 | 0.40 | 0.85 | |||
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0.1863 | 4.36 | 0.37 | 1 (1) | ≲ 10 500 | 286 | 0.50 | 0.74 |
2 (1) | 10 200−9000 | 355 | 0.60 | 0.62 | |||
1 (2) | ≲ 10 500 | 168 | 0.57 | 0.65 | |||
2 (2) | 10 200−9000 | 219 | 0.68 | 0.54 | |||
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0.1917 | 4.49 | 0.35 | 1 (1) | ≲ 10 500 | 280 | 0.45 | 0.78 |
2 (1) | ≲ 10 220 | 340 | 0.72 | 0.49 | |||
1 (2) | ≲ 10 500 | 160 | 0.57 | 0.61 | |||
2 (2) | ≲ 8900 | 210 | 2.60 | 0.13 | |||
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0.2019 | 3.80 | 0.32 | 1 (1) | ≲ 10 600 | 263 | 0.09 | 3.6 |
1 (2) | ≲ 10 590 | 155 | 0.25 | 1.28 | |||
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0.2389 | 3.61 | 0.62 | 1 (1) | ≲ 10 700 | 200 | 0.04 | 15.5 |
2 (1) | 10 500−7620 | 300 | 0.15 | 4.1 | |||
1 (2) | ≲ 10 700 | 120 | 0.06 | 10.3 | |||
2 (2) | 10 500−9000 | 180 | 0.07 | 8.9 |
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