Table 1.
Characteristics of 1.5 M⊙ magneto-rotational models.
Prot, ini | Bp, ini | τMS | ΔMMS | ⟨Ṁ⟩MS | τbreak, ZAMS | η*, ZAMS | Prot, TAMS | Bp, TAMS | JTAMS/JZAMS |
---|---|---|---|---|---|---|---|---|---|
(d) | (G) | (Gyr) | (M⊙) | (M⊙ yr−1) | (Gyr) | – | (d) | (G) | – |
1.00 | 10.00 | 2.73 | −1.33e−02 | −4.86e−12 | 20.12 | 0.24 | 2.24 | 0.05 | 0.82 |
1.00 | 100.00 | 2.67 | −8.26e−03 | −3.09e−12 | 3.90 | 23.74 | 2.59 | 0.62 | 0.73 |
1.00 | 1.00e+03 | 2.58 | −1.78e−03 | −6.91e−13 | 0.45 | 2.64e+03 | 55.68 | 23.93 | 0.04 |
1.00 | 1.00e+04 | 2.88 | −3.43e−04 | −1.19e−13 | 0.03 | 7.51e+05 | Inf. | 9.76e+02 | 0. |
10.00 | 10.00 | 2.70 | −8.30e−03 | −3.07e−12 | 9.44 | 2.89 | 22.91 | 0.56 | 0.80 |
10.00 | 100.00 | 2.63 | −2.87e−03 | −1.09e−12 | 1.45 | 2.81e+02 | 69.81 | 8.35 | 0.28 |
10.00 | 1.00e+03 | 2.49 | −6.47e−04 | −2.60e−13 | 0.15 | 3.54e+04 | 1.22e+10 | 182.46 | 2.18e−09 |
10.00 | 1.00e+04 | 2.94 | −2.18e−04 | −7.41e−14 | 1.02e−02 | 6.41e+06 | Inf. | 2.40e+03 | 0. |
100.00 | 10.00 | 2.71 | −6.04e−03 | −2.23e−12 | 6.72 | 7.74 | 2.63e+02 | 1.40 | 0.70 |
100.00 | 100.00 | 2.59 | −1.87e−03 | −7.23e−13 | 0.87 | 8.68e+02 | 3.30e+03 | 18.41 | 0.06 |
100.00 | 1.00e+03 | 2.44 | −5.31e−04 | −2.18e−13 | 0.09 | 1.11e+05 | 8.47e+14 | 2.30e+02 | 3.73e−13 |
100.00 | 1.00e+04 | 2.95 | −2.07e−04 | −7.01e−14 | 7.26e−03 | 1.31e+07 | Inf. | 2.50e+03 | 0. |
1.00e+03 | 10.00 | 2.71 | −5.85e−03 | −2.16e−12 | 6.47 | 8.97 | 2.68e+03 | 1.48 | 0.69 |
1.00e+03 | 100.00 | 2.58 | −1.83e−03 | −7.08e−13 | 0.81 | 1.02e+03 | 3.72e+04 | 19.33 | 0.05 |
1.00e+03 | 1.00e+03 | 2.44 | −5.30e−04 | −2.17e−13 | 0.08 | 1.34e+05 | 1.07e+16 | 2.30e+02 | 3.10e−13 |
1.00e+03 | 1.00e+04 | 2.96 | −2.09e−04 | −7.05e−14 | 7.09e−03 | 1.38e+07 | Inf. | 2.48e+03 | 0. |
Notes. τMS is the main-sequence lifetime, ΔMMS is the total mass lost during the MS phase, ⟨Ṁ⟩MS = ΔMMS/τMS is the averaged mass loss rate for the MS phase, is the braking timescale measured at ZAMS, η*, ZAMS is the magnetic confinement parameter at ZAMS, and Prot, TAMS, Bp, TAMS, and JTAMS are the rotation period, the field strength at the pole, and the total angular momentum at TAMS.
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