2007
DOI: 10.1134/s106377370702003x
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Hydrodynamic processes of angular momentum transport in the interior of a rotating massive hydrogen-burning star

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Cited by 9 publications
(17 citation statements)
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“…The flux of hydrogen from the radiative turbulent envelope into the convective core has its maximum in the second half of the star's evolution along the main sequence [25]. The intensity of hydrodynamic transport processes in the non-convective layers of a star is determined by the momentum and Schmidt number in the turbulent radiative envelope [25,26], and can be different for stars of the same mass. For example, the mass of the chemically homogeneous region in the central part of the star during the second half of its main-sequence evolution is determined by the combined action of turbulent entrainment and shear turbulence, and can be different for stars of the same mass.…”
Section: Results Of the Computationsmentioning
confidence: 99%
“…The flux of hydrogen from the radiative turbulent envelope into the convective core has its maximum in the second half of the star's evolution along the main sequence [25]. The intensity of hydrodynamic transport processes in the non-convective layers of a star is determined by the momentum and Schmidt number in the turbulent radiative envelope [25,26], and can be different for stars of the same mass. For example, the mass of the chemically homogeneous region in the central part of the star during the second half of its main-sequence evolution is determined by the combined action of turbulent entrainment and shear turbulence, and can be different for stars of the same mass.…”
Section: Results Of the Computationsmentioning
confidence: 99%
“…The evolution of an isolated star with a mass of 16 M ⊙ and an angular momentum J in the range 0.92 × 10 52 − 3.69 × 10 52 erg • s was studied on the main sequence (Staritsin 2007). The inner part of a star with a mass of 10.7 M ⊙ contains 47% of the angular momentum of the star at J = 0.92×10 52 erg•s and 34% at J = 3.69 × 10 52 erg • s, when the hydrogen content in the convective core is the same as in the accretor.…”
Section: Discussionmentioning
confidence: 99%
“…Turbulent viscosity coefficients have been determined by Talon and Zahn (1997), Maeder (2003), and Mathis et al (2004). Equations ( 3) and ( 4) are solved along with equations of stellar structure and evolution (Staritsin 1999(Staritsin , 2005(Staritsin , 2007(Staritsin , 2014.…”
Section: Angular Momentum Transfer In the Accretormentioning
confidence: 99%
“…To solve Eq. ( 6), a difference scheme based on the integrointerpolation method (Samarskij & Popov 1992) was elaborated (Staritsin 1999(Staritsin , 2005(Staritsin , 2007. The method implies an integration of Eq.…”
Section: Transport Of Angular Momentummentioning
confidence: 99%
“…Be type stars exhibit the following properties: emission in the Balmer lines of hydrogen, excess radiation in the infrared part of the spectrum, and rapid rotation (Porter & Rivinius 2003). There are several channels by which a Be star can acquire a fast rotation: the process of star birth, the removal of angular momentum from the interior of an isolated star to the exterior during evolution along the main sequence (Meynet & Maeder 2005;Staritsin 2007Staritsin , 2009Ekstrom et al 2008;Granada & Haemmerle 2014;Gagnier et al 2019), mass and angular momentum exchange in a binary system in the Hertzsprung gap (Pols et al 1991;Portegies Zwart 1995;Van Bever & Vanbeveren 1997), or the merging of a pair of main sequence stars (Shao & Li 2014).…”
Section: Introductionmentioning
confidence: 99%