@Article{LundWFVSBJK:2019:RaHySi,
author = "Lund, Kristin and Wood, K. and Falceta-Gon{\c{c}}alves, Diego and
Vandenbroucke, Bert and Sartorio, Nina Sanches and Bonnell, I. A.
and Johnston, K. G. and Keto, E.",
affiliation = "{University of St Andrews} and {University of St Andrews} and
{University of St Andrews} and {University of St Andrews} and
{Instituto Nacional de Pesquisas Espaciais (INPE)} and {University
of St Andrews} and {The University of Leeds} and
{Harvard-Smithsonian Center for Astrophysics}",
title = "Radiation hydrodynamic simulations of massive star formation via
gravitationally trapped H II regions – spherically symmetric
ionized accretion flows",
journal = "Monthly Notices of the Royal Astronomical Society",
year = "2019",
volume = "485",
number = "3",
pages = "3761--3770",
month = "May",
keywords = "hydrodynamics, radiative transfer, stars: formation, stars:
massive, H II regions.",
abstract = "This paper investigates the gravitational trapping of H II regions
predicted by steady-state analysis using radiation hydrodynamical
simulations. We present idealized spherically symmetric radiation
hydrodynamical simulations of the early evolution of H II regions
including the gravity of the central source. As with analytic
steady-state solutions of spherically symmetric ionized Bondi
accretion flows, we find gravitationally trapped H II regions with
accretion through the ionization front on to the source. We found
that, for a constant ionizing luminosity, fluctuations in the
ionization front are unstable. This instability only occurs in
this spherically symmetric accretion geometry. In the context of
massive star formation, the ionizing luminosity increases with
time as the source accretes mass. The maximum radius of the
recurring H II region increases on the accretion time-scale until
it reaches the sonic radius, where the infall velocity equals the
sound speed of the ionized gas, after which it enters a
pressure-driven expansion phase. This expansion prevents accretion
of gas through the ionization front, the accretion rate on to the
star decreases to zero, and it stops growing from accretion.
Because of the time required for any significant change in stellar
mass and luminosity through accretion our simulations keep both
mass and luminosity constant and follow the evolution from trapped
to expanding in a piecewise manner. Implications of this evolution
of H II regions include a continuation of accretion of material on
to forming stars for a period after the star starts to emit
ionizing radiation, and an extension of the lifetime of
ultracompact H II regions.",
doi = "10.1093/mnras/stz621",
url = "http://dx.doi.org/10.1093/mnras/stz621",
issn = "0035-8711 and 1365-2966",
language = "en",
targetfile = "lund_radiation.pdf",
urlaccessdate = "27 abr. 2024"
}