Chandra X-ray Observatory - HomeAbout The ChandraEducational MaterialsField GuidePhoto AlbumPress RoomResources
Chandra X-ray Observatory - HomeChandra Field Guide - You are here
ObservatoryAbout X-ray AstronomyX-Ray SourcesSolar SystemNormal Stars & Star ClustersWhite Dwarfs & Planetary NebulasSupernovas & Supernova RemnantsNeutron Stars/X-ray BinariesBlack HolesNormal Galaxies & Starburst GalaxiesQuasars & Active GalaxiesGroups & Clusters of GalaxiesCosmology/Deep Fields/X-ray BackgroundMiscellaneousBrown Dwarfs Gamma Ray Bursts
Web Site ToolsVisit the Chandra ChroniclesEmail NewsletterSite MapNew & NoteworthyImage Use PolicyQuestions & AnswersGlossaryDownload Guide

Mid-mass Black Holes

Schematic of a Black Hole
Schematic of
a Black Hole
There is strong evidence for two types of black holes: stellar black holes with masses of a dozen or so Suns, and supermassive black holes with masses of many millions of Suns. Stellar black holes are formed as a natural consequence of the evolution of massive stars. The origin of supermassive black holes is a mystery. They are found only in the centers of galaxies. It is not known whether they formed in the initial collapse of the gas cloud that formed the galaxy, or from the gradual growth of a stellar mass black hole, or from the merger of a centrally located cluster of black holes, or by some other mechanism.

radiation pressure balance schematic
Radiation Pressure Schematic
When matter is pulled toward a black hole,
it is heated and produces X-rays. These
X-rays create a radiation pressure which
pushes out on the matter. If the matter
continues to fall in,the radiation pressure
of the X-rays must be less than the pull of
the black hole's gravity. This effect, called
the Eddington limit, enables astronomers to
estimate the mass of a black hole.
The mass of a stellar black hole can be deduced by observing the orbital acceleration of a star as it orbits its unseen companion. Likewise, the mass of a supermassive black hole can be determined by using the orbital acceleration of gas clouds swirling around the central black hole. When orbital acceleration cannot be used to establish the mass of a black hole, astronomers can place a lower limit on its mass by measuring the X-ray luminosity due to matter falling into a black hole. The pressure of the outflowing X-rays must be less than the pull of the black hole's gravity on the inflowing matter.


Page 1 | 2


separator line
CXC Home | Search | Help | Site Map | Image Use Policy | Privacy & Accessibility | Downloads & Plugins
Latest Images | New & Noteworthy | Multimedia | Flash Ecards | Glossary | Q&A | Guestbook


RSS Feed RSS Feed | Podcast Podcast | Blog Blog

[News by email: Chandra Digest]
[Contact us: cxcpub@cfa.harvard.edu]
NASA's Home Page Smithsonian's Home Page CXC Home Page Image Map for NASA's, Smithsonian and Chandra's Home Pages
Harvard-Smithsonian Center for Astrophysics
60 Garden Street, Cambridge, MA 02138 USA
Phone: 617.496.7941 Fax: 617.495.7356


Text Size:
normal font large font larger font
Chandra X-ray Center, Operated for NASA by the Smithsonian Astrophysical Observatory
This site was developed with funding from NASA under Contract NAS8-03060.
Revised: August 29, 2006