AFGL 2298

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AFGL 2298

A near-infrared (J band) light curve for AFGL 2298, adapted from Clark et al. (2009)[1]
Observation data
J2000
Constellation Aquila
Right ascension 19h 00m 10.89s[2]
Declination +03° 45′ 47.1″[2]
Characteristics
Spectral type B8I,[3] B:I:[e],[4] B0-0.5I[5]
Apparent magnitude (J) 12.164[2]
Apparent magnitude (H) 8.918[2]
Apparent magnitude (K) 6.91[6]
Variable type LBV[4]
Distance
30,000±10,000 ly
(10,000±3,000[4] pc)
Absolute bolometric
magnitude
 (Mbol)
−11.25[1]
Details
Radius158 - 385[1] R
Luminosity1,300,000 - 2,000,000[1] L
Temperature11,000 - 15,500[1] or 26,000[5] K
V1672 Aql, RAFGL 2298, IRAS 18576+0341, 2MASS J19001089+0345471[7]
Database references
SIMBADdata

AFGL 2298, also known as IRAS 18576+0341, is a

interstellar extinction, so its apparent magnitude is brighter for longer-wavelength passbands; in fact, in visual wavelengths it is completely undetectable.[7]

AFGL 2298 has an

bolometric magnitude of −11.25,[1] making it one of the most luminous stars known. Indeed, many of the hottest and most luminous stars known are luminous blue variables and other early-type stars. However, like all LBVs, AFGL 2298 is highly variable and the bolometric magnitude refers to its peak luminosity.[1] Its status as an LBV was confirmed in 2003.[4]

Like most extremely massive stars, AFGL 2298 is undergoing mass loss.[5] For example, in 2005 it was estimated to be losing 3.7×10−5 solar masses each year,[5] although the rate of mass loss itself varies frequently and dramatically.[1] The stellar mass is currently being ejected as a nebula around the star (similar to AG Carinae), which was imaged by the Very Large Telescope in 2010.[8] The nebula was found to be fairly circular, and the properties of the dust appeared to be constant throughout the entire nebula.[8]

Properties of AFGL 2298 over time[1]
Effective temperature (K) Mass loss rate (M/yr) Bolometric luminosity (L)
June 2001 11,700 4.5×10−5 1.5×106
August 2002 10,900 1.2×10−4 1.3×106
June 2006 10,300 5.2×10−5 2.0×106
May 2007 10,900 4×10−5 1.5×106

See also

References