2022
DOI: 10.1093/mnras/stac1654
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A semi-analytical model for the temporal evolution of the episodic disc-to-star accretion rate during star formation

Abstract: We develop a semi-analytic formalism for the determination of the evolution of the stellar mass accretion rate for specified density and velocity profiles that emerge from the runaway collapse of a prestellar cloud core. In the early phase, when the infall of matter from the surrounding envelope is substantial, the star accumulates mass primarily because of envelope-induced gravitational instability in a protostellar disc. In this phase, we model the envelope mass accretion rate from the isothermal free-fall c… Show more

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Cited by 4 publications
(2 citation statements)
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“…During the embedded phase, envelope accretion and viscous processes naturally increase a disk's mass and size as the angular momentum is redistributed. However, when a disk becomes too massive, it can become gravitationally unstable, forming asymmetries and spiral features (e.g., Kuffmeier et al 2018) and sometimes fragmenting (e.g., Vorobyov & Basu 2006;Das & Basu 2022). The Toomre Q parameter (Toomre 1964) is a standard metric used to determine whether a disk is gravitationally stable (Q  1) or unstable (Q  1).…”
Section: Envelope Infall Versus Stellar Accretion Ratementioning
confidence: 99%
“…During the embedded phase, envelope accretion and viscous processes naturally increase a disk's mass and size as the angular momentum is redistributed. However, when a disk becomes too massive, it can become gravitationally unstable, forming asymmetries and spiral features (e.g., Kuffmeier et al 2018) and sometimes fragmenting (e.g., Vorobyov & Basu 2006;Das & Basu 2022). The Toomre Q parameter (Toomre 1964) is a standard metric used to determine whether a disk is gravitationally stable (Q  1) or unstable (Q  1).…”
Section: Envelope Infall Versus Stellar Accretion Ratementioning
confidence: 99%
“…The solution of the disk evolution after protostar formation consists of a highly episodic accretion process. While some features of the episodes can be understood in a deterministic manner using the criterion for gravitational instability (Das & Basu 2022), the nonaxisymmetry and nonlinearity of the problem lead to a time evolution of accretion rate that has stochastic and chaotic features. Each simulation is quite costly in terms of run time (up to several months on a single computer node with 48 physical cores), and a typical parameter survey consists of ∼ 10 models.…”
Section: Hydrodynamic Simulationsmentioning
confidence: 99%