HD 269810
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| Observation data Epoch J2000 Equinox J2000 |
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|---|---|
| Constellation | Dorado |
| Right ascension | 05h 35m 13.9s |
| Declination | −67° 33′ 27.5″ |
| Apparent magnitude (V) | 12.22[1] |
| Characteristics | |
| Spectral type | O2III(f*)[2] |
| B−V color index | −0.14[1] |
| Variable type | None |
| Astrometry | |
| Radial velocity (Rv) | 303[3] km/s |
| Proper motion (μ) | RA: 0.9[4] mas/yr Dec.: -0.9[4] mas/yr |
| Absolute magnitude (MV) | −6.6[2] |
| Details | |
| Mass | 130[2] M☉ |
| Radius | 18[5] R☉ |
| Luminosity | 2.2 million[2] L☉ |
| Surface gravity (log g) | 4.0[2] cgs |
| Temperature | 52,500[2] K |
| Metallicity | ≤0.1[2] He/H |
| Rotation | 173[6] |
| Other designations | |
| Database references | |
| SIMBAD | data |
HD 269810 is a blue giant star in the Large Magellanic Cloud. It is one of the most massive and most luminous stars known, and one of only a handful of stars with the spectral type O2.
Name
The star's name, HD 269810, comes from the Henry Draper Catalogue. The serial number 269810 indicates it was published in the extension of the catalogue and is formally referred to as HDE 269810.
Details
HD 269810 is classified as an O2III(f*) star with a temperature of 52,500 K (52,200 °C; 94,000 °F). The luminosity class of III indicates a star somewhat evolved and expanded compared to the zero age main sequence. The spectral peculiarity code (f*) indicates strong NIII emission lines, even stronger NNIV emission, and weak HeNII emission. The star is 18 R☉, but because of its high surface temperature it is two million times brighter than the Sun. The high temperature generates a fast stellar wind of 3,750 km/s (2,330 mi/s),[7] shedding over a millionth of the mass of the sun each year.[2] In 1995, HD 269810 was estimated to be 190 times the mass of the Sun[8] and was thought to be the heaviest star known, but the mass is now thought to be around 130 M☉.[2]
Evolution
Stars as massive as HD 269810 with metallicity typical of the Large Magellanic Cloud will maintain near-homogeneous chemical structure due to strong convection and rotational mixing. This produces strong helium and nitrogen surface abundance enhancement even during core hydrogen burning. Their rotation rates will also decrease significantly due to mass loss and envelope inflation, so that gamma-ray bursts are unlikely when this type of star reaches core collapse. They are expected to develop directly into Wolf–Rayet stars, passing through WN, WC, and WO stages before exploding as a type Ic supernova and leaving behind a black hole. The total lifetime would be around 2 million years, showing an O-type spectrum for most of that time before a shorter period with a WR spectrum.[9][10]
References
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