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首页> 外文期刊>Astronomy and astrophysics >Grids of stellar models with rotation - I. Models from 0.8 to 120?M⊙ at solar metallicity (Z = 0.014)
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Grids of stellar models with rotation - I. Models from 0.8 to 120?M⊙ at solar metallicity (Z = 0.014)

机译:带有旋转的恒星模型的网格-I.太阳金属度(Z = 0.014)时从0.8到120?M⊙的模型

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Aims. Many topical astrophysical research areas, such as the properties of planet host stars, the nature of the progenitors of different types of supernovae and gamma ray bursts, and the evolution of galaxies, require complete and homogeneous sets of stellar models at different metallicities in order to be studied during the whole of cosmic history. We present here a first set of models for solar metallicity, where the effects of rotation are accounted for in a homogeneous way. Methods. We computed a grid of 48 different stellar evolutionary tracks, both rotating and non-rotating, at Z?=?0.014, spanning a wide mass range from 0.8 to 120?M⊙. For each of the stellar masses considered, electronic tables provide data for 400 stages along the evolutionary track and at each stage, a set of 43 physical data are given. These grids thus provide an extensive and detailed data basis for comparisons with the observations. The rotating models start on the zero-age main sequence (ZAMS) with a rotation rate υini/υcrit?=?0.4. The evolution is computed until the end of the central carbon-burning phase, the early asymptotic giant branch (AGB) phase, or the core helium-flash for, respectively, the massive, intermediate, and both low and very low mass stars. The initial abundances are those deduced by Asplund and collaborators, which best fit the observed abundances of massive stars in the solar neighbourhood. We update both the opacities and nuclear reaction rates, and introduce new prescriptions for the mass-loss rates as stars approach the Eddington and/or the critical velocity. We account for both atomic diffusion and magnetic braking in our low-mass star models. Results. The present rotating models provide a good description of the average evolution of non-interacting stars. In particular, they reproduce the observed main-sequence width, the positions of the red giant and supergiant stars in the Hertzsprung-Russell (HR) diagram, the observed surface compositions and rotational velocities. Very interestingly, the enhancement of the mass loss during the red-supergiant stage, when the luminosity becomes supra-Eddington in some outer layers, help models above 15?20?M⊙ to lose a significant part of their hydrogen envelope and evolve back into the blue part of the HR diagram. This result has interesting consequences for the blue to red supergiant ratio, the minimum mass for stars to become Wolf-Rayet stars, and the maximum initial mass of stars that explode as type?II?P supernovae.
机译:目的许多主题的天体物理学研究领域,例如行星宿主恒星的特性,不同类型的超新星和伽马射线爆发的祖先的性质以及星系的演化,都需要在不同金属度下完整且均匀的恒星模型集,以便在整个宇宙历史中被研究。我们在这里介绍了第一组关于太阳金属性的模型,其中以同质的方式解释了旋转的影响。方法。我们计算出一个由48个不同的恒星演化轨道组成的网格,这些轨道分别在Z?=?0.014时旋转和不旋转,其质量范围从0.8到120?M⊙。对于所考虑的每个恒星质量,电子表提供了沿演化轨迹的400个阶段的数据,并且在每个阶段都给出了43个物理数据的集合。因此,这些网格为与观测值的比较提供了广泛而详细的数据基础。旋转模型从零年龄主序列(ZAMS)开始,旋转速率υini/υcrit?=?0.4。计算演化过程直到中心碳燃烧阶段,早期渐近巨型分支(AGB)阶段或核心氦闪,分别针对质量,中间质量以及低质量和极低质量的恒星。最初的丰度是由Asplund和合作者推论得出的,最适合于太阳附近地区观测到的大质量恒星的丰度。我们更新了不透明性和核反应速率,并为恒星接近爱丁顿和/或临界速度引入了质量损失率的新规定。在我们的低质量恒星模型中,我们同时考虑了原子扩散和电磁制动。结果。当前的自转模型很好地描述了非相互作用恒星的平均演化。特别是,它们再现了观察到的主序宽度,赫兹普劳-罗素(HR)图中红色巨星和超巨型恒星的位置,观察到的表面成分和旋转速度。非常有趣的是,在红色超巨星阶段,当某些外层的光度变为超爱丁顿时,质量损失增加,这有助于模型在15?20?M⊙以上损失掉大部分的氢包层并演变成人力资源图的蓝色部分。这个结果对蓝色到红色的超巨星比率,成为沃尔夫-雷耶特星的恒星的最小质量以及作为II?P型超新星爆炸的恒星的最大初始质量具有有趣的影响。

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