SearcharxivSearch

arXiv · astro-ph/9610131

Heating of a Star by Disk Accretion

Abstract

We examine various ways in which disk accretion can heat an accreting star. These include 1) radiation emitted from the disk surface which is intercepted by the stellar surface, 2) radiative flux directly across the disk-star interface, and 3) advection of thermal energy from the disk into the star. For each of these, the physics of the boundary layer between the disk and the star is crucial to determining the amount of stellar heating that occurs. We assess the importance of the methods listed above for heating the star in accreting pre-main-sequence stars and cataclysmic variables, using recent models of boundary layers in these systems. We find that intercepted radiation tends to be the most important source of stellar heating in thin disk systems such as T Tauri stars and high-$\dot M$ cataclysmic variables. We argue that direct radiation across the disk-star interface will be unimportant in steady-state systems. However, it may be important in outbursting systems, where the disk temperature rises and falls rapidly. Advection of thermal energy into the star becomes the dominant source of stellar heating in thick disk systems such as FU Orionis objects.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Robert Popham. 1996-10-16. Heating of a Star by Disk Accretion. https://doi.org/10.1086/303806

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Deformation procedure for scalar fields in cosmology

This work offers an extension of the deformation procedure introduced in field theory to the case of standard cosmology in the presence of real scalar field in flat space-time. The procedure is shown to work for many models, which give rise to several different cosmic scenarios, evolving under the presence of first-order differential equations which solve the corresponding equations of motion very appropriately.

astro-ph

Dark Energy is the Cosmological Quantum Vacuum Energy of Light Particles-The Axion and the Lightest Neutrino

We uncover the general mechanism producing the dark energy(DE). This is only based on well known quantum physics and cosmology. We show that the observed DE originates from the cosmological quantum vacuum of light particles which provides a continuous energy distribution able to reproduce the data. Bosons give positive contributions to the DE while fermions yield negative contributions. As usual in field theory, ultraviolet divergences are subtracted from the physical quantities. The subtractions respect the symmetries of the theory and we normalize the physical quantities to be zero for the Minkowski vacuum. The resulting finite contributions to the energy density and the pressure from the quantum vacuum grow as log a(t) where a(t) is the scale factor, while the particle contributions dilute as 1/a^3(t), as it must be for massive particles. The DE equation of state P = w(z)H turns to be w(z)<-1 with w(z) asymptotically reaching the value -1 from below.A scalar particle can produce the observed DE through its quantum cosmological vacuum provided:(i)its mass is of the order of 10^{-3} eV = 1 meV,(ii) it is very weakly coupled and (iii) it is stable on the time scale of the age of the universe. The axion vacuum thus appears as a natural candidate. The neutrino vacuum (especially the lightest mass eigenstate) can give negative contributions to the DE. We find that w(z=0) is slightly below -1 by an amount ranging from [-1.5 10^{-3}] to [-8 10^{-3}] and we predict the axion mass to be in the range between 4 and 5 meV. We find that the universe will expand in the future faster than the de Sitter universe, as an exponential in the square of the cosmic time. DE arises from the quantum vacua of light particles in FRW cosmological space time in an analogous way to the Casimir effect in Minkowski spacetime with non trivial boundaries.

astro-ph