Skip to main content

STELLAR WIND NEAR MASSIVE BLACK HOLES

Image: X-rays from Chandra in blue and infrared emission from the Hubble Space Telescope in red and yellow. The inset shows a close-up view of Sgr A* in X-rays only, covering a region half a light year wide. The diffuse X-ray emission is from hot gas captured by the black hole and being pulled inwards. This hot gas originates from winds produced by a disk-shaped distribution of young massive stars observed in infrared observations. Credit: X-ray: NASA/UMass/D.Wang et al., IR: NASA/STScI

Within the central tenth of a parsec in the middle of our galaxy there is a concentration of young stars (S-stars) that interact with a supermassive black hole Sagittarius A* (Sgr A*).


The S-stars in the galactic center are thought to be massive, early B-type stars and therefore should exhibit hot stellar winds. These winds provide gaseous material that can be accreted by the black hole which is thought to be the source of X-ray emission close to Sgr A*.

Image: Morgan-Keenan-Kellman spectral classification of main-sequence stars (Sun - type G).
Credit: LucasVB / Wikimedia.
In contrast to gas, the orbits of the stars are governed by gravitation only and therefore provide an excellent tracer for the gravitational potential in our Galactic center. This unique setup provides the best measurement of the mass of a black hole to date and unambiguously confirms the existence of a supermassive black hole in the center of our galaxy.

In a recent paper (Lutzgendorf et al 2016), the authors simulate the gravitational physics, stellar evolution and hydrodynamics of the S-stars orbiting the supermassive black hole, and they use this framework to determine the amount of gas that is accreted onto the black hole.

Image: snapshots at 6 different times in the simulation. The images are centered on the black hole (white cross). The initial position of the stars are marked in the first panel with green circles. Credit: Lutzgendorf et al 2016.

They found that the accretion rate is sensitive to the wind properties of the S-stars, and that the simulations are consistent with the observed accretion rate of Sgr A* (~10^{-6} solar masses/year) only if the stars exhibit high wind massloss rates that are comparable with those of evolved 7-10 Myr old stars with masses of M=19-25 solar masses. This result is in contrast with observations that have shown that these stars are rather young, main-sequence B-stars.
The authors conclude that the S-stars in their present stage are not the main contributors to the accretion rate of Sgr A* and the inflow of gas from the massive O-stars (located farther from Sgr A*) is needed.

(Animation of the simulation - Lutzgendorf et al 2016)

The paper (Lutzgendorf et al 2016) is available online and is published in the MNRAS. >>
http://arxiv.org/abs/1512.03304
http://mnras.oxfordjournals.org/content/456/4/3645.abstract

Comments

Popular posts from this blog

A METHOD TO TEST THE EXISTENCE OF REGULAR BLACK HOLES

Illustration of a black hole. Image Credit & Copyright: Alain Riazuelo The existence of the singularity is an intrinsic problem of the General Relativity (GR). At the fundamentally level, the resolution of the problem of the singularity lies with the expectation that under situations where quantum effects become strong, the behavior of gravity could possibly greatly deviate from that predicted by the classical theory of GR. Regular black hole solution are proposed with the same spacetime geometry outside the horizon as the traditional black hole, but bears no singularity inside. Whether or not black hole singularities should exist, they would be covered by the black hole horizon. The black hole horizon serves as an information curtain hindering outside observers from directly observing the interior structure of the black hole, and determining that whether or not the black hole singularity does really exist. A method is needed to check the correctness of the new constructions ...

ORBITAL PERIODS OF THE PLANETS

For orbital period generally we refer to the sidereal period, that is the temporal cycle that it takes an object to make a full orbit, relative to the stars. This is the orbital period in an inertial (non-rotating) frame of reference (365,25 days for the earth).

Astrophysics collection (March 11, 2016)

Latest astrophysics news Rotation curves of galaxies as a test of MOND? Galaxies are rotating with such speed that the gravity generated by their observable matter could not possibly hold them together. In a recent paper ( Haghi et al. 2016 ) the authors test the Modified Newtonian Dynamics (MOND).    Read>> A binary origin for a central compact object (CCO)? Doroshenko et al. 2016 investigate the possible binary origin of the CCO XMMUJ173203.3-344518 .   Read>> Rapidly rotating pulsars as possible sources of fast radio bursts (FRB) In a recent paper ( Lyutikov et al. 2016 ) the authors discuss possible association of fast radio bursts (FRBs) with supergiant pulses emitted by young pulsars.   Read>> Supernovae from WD-WD direct collisions In recent years it was suggested that WD-WD direct collisions (probably extremely rare and occurring only in dense stellar clusters) provide an additional channel for supernova...