List of most massive known stars

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This is a list of the most-massive stars so far discovered, in solar masses (M).

Uncertainties and caveats[edit]

Most of the masses listed below are contested and, being the subject of current research, remain under review and subject to revision.

The masses listed in the table below are inferred from theory, using difficult measurements of the stars’ temperatures and absolute brightnesses. All the listed masses are uncertain: both the theory and the measurements are pushing the limits of current knowledge and technology. Either measurement or theory, or both, could be incorrect. For example, VV Cephei could be between 25–40 M, or 100 M, depending on which property of the star is examined.

Artist's impression of disc of obscuring material around a massive star.

Massive stars are rare; astronomers must look very far from the Earth to find one. All the listed stars are many thousands of light years away and that alone makes measurements difficult. In addition to being far away, many stars of such extreme mass are surrounded by clouds of outflowing gas; the surrounding gas interferes with the already difficult-to-obtain measurements of stellar temperatures and brightnesses and greatly complicates the issue of estimating internal chemical compositions. For some methods, different determinations of chemical composition lead to different estimates of mass. In addition, the clouds of gas make it difficult to judge whether the star is just a single supermassive object or, instead, a multiple star system. A number of the "stars" listed below may actually consist of two or more companions in close orbit, each star being massive in itself but not necessarily supermassive. Other combinations are possible – for example a supermassive star with one or more smaller companions or more than one giant star. Without being able to see inside the surrounding cloud, it is difficult to know the truth of the matter.

Amongst the most reliable listed masses are those for NGC 3603-A1, WR21a and WR20a, which were obtained from orbital measurements. These entities are members of (different) binary star systems and it is possible to measure in both cases the individual masses of the two stars by studying their orbital motions, using Kepler's laws of planetary motion. This involves measuring their radial velocities and also their light curves, as they are eclipsing binaries. The derivation of binary masses requires relatively limited information about the orbital parameters but one key value that isn't always accurately known is the inclination. Without this only a minimum value for the masses can be derived, so several binaries are shown with masses as greater than a particular value. For eclipsing binaries, the inclination can be derived with better accuracy. The list gives only the inferred masses of stars according to recent best estimates and does not include superseded estimates of mass.

Relevance of stellar evolution[edit]

Some stars may once have been heavier than they are today. It is likely that many have lost tens of solar masses of material in the process of degassing, or in sub-supernova and supernova impostor explosion events.

There are also – or rather were – stars that might have appeared on the list but no longer exist as stars. Today we see only the debris (see for example hypernovae and supernova remnant). The masses of the precursor stars that fueled these cataclysms can be estimated from the type of explosion and the energy released, but those masses are not listed here.

List of the most massive stars[edit]

Known stars with an estimated mass of 25 or greater M. Masses are their current (evolutionary) mass, not their initial (formation) mass. The list is far from complete, although the majority of stars thought to be more than 100 M are shown.

Star name Mass
(M, Sun = 1)
R136a1 [1] 256
BAT99-98[2] 226
R136a2 [1] 179
VFTS 682 150
NGC 3603-B[1] 132
R136a3 [2] 130
HD 269810 130
WR42e[3] 125-135[a]
Arches-F9 111–131
η Carinae A 120
NGC 3603-A1 116 + 89
Arches-F1 101–119
Arches-F6 111–131
R145[4] >116 + >48[b]
HD 93250 118
NGC 3603-C[1] 113
Melnick 42 113
Cygnus OB2-12 110
Peony Star[5] 100
R136c [2] 99
Arches-F7 86–102
Cluster R136a About 20 more stars around 100
HD 93129 A 95
WR21a[6] A=87, B=53
The Pistol Star 86-92
WR20a A=83, B=82
Arches-F15 80–97
Sk -71 51[7] 80
R139[8] A=78, B=66
V429 Carinae A + B A=78, B=21
Pismis 24-17[9] 78
R126 70
Companion to M33 X-7[10] 70
Pismis 24-1SW 66
LBV 1806-20 A + B A=65, B=65
LY Aurigae 64
Var 83 in M33 60–85
HD 148937[11] 60
HD 5980 A + B A=58-79, B=51-67
CD Crucis A + B[12] A=57, B=48
Plaskett's star A=54, B=56
HD 93129B[13] 52
AG Carinae 50
LH54-425 A + B[14] A=47, B=28
WR102c[5] 45–55
S Doradus 45
IRS-8*[15] 44.5
Sher 25 in NGC 3603 40–52
DL Crucis 40–50
α Camelopardalis 43
χ2 Orionis 42.3
ε Orionis 40
ρ Cassiopeiae 40
RW Cephei 40
θ1 Orionis C 40
V382 Carinae 39
Companion to NGC 300 X-1[16] 38
ζ1 Scorpii 36
Companion to IC 10 X-1[17] 35
ν Aquilae 30–45
19 Cephei 30–35
γ Velorum A 30
P Cygni 30
R 66 30
η Canis Majoris 30
ζ Orionis 28
IRS 15[18] 26
VV Cephei 25–40
ξ Persei 26–36
6 Cassiopeiae[19] 25
EZ Canis Majoris 25
KY Cygni 25
μ Cephei 25
V509 Cassiopeiae 25
NGC 7538 S[20] 25
S Monocerotis A 18–30
ζ Puppis 22.5
  1. ^ This unusual measurement was made by assuming the star was ejected from a three-body encounter in NGC 3603. This assumption also means that the current star is the result of a merger between two original close binary components. The mass is consistent with evolutionary mass for a star with the observed parameters.
  2. ^ These are minimum values with the orbital solution still uncertain.

Black holes[edit]

Black holes are the end point evolution of massive stars. Technically they are not stars, as they no longer generate heat and light via nuclear fusion in their cores.

Eddington's size limit[edit]

Main article: Eddington luminosity

The limit on mass arises because stars of greater mass have a higher rate of core energy generation, their luminosity increasing far out of proportion to their mass. For a sufficiently massive star the outward pressure of radiant energy generated by nuclear fusion in the star’s core exceeds the inward pull of its own gravity. This is called the Eddington limit. Beyond this limit, a star ought to push itself apart, or at least shed enough mass to reduce its internal energy generation to a lower, maintainable rate. In theory, a more massive star could not hold itself together, because of the mass loss resulting from the outflow of stellar material. In practice the theoretical Eddington Limit must be modified for high luminosity stars and the empirical Humphreys Davidson Limit is derived.[21]

Astronomers have long theorized that as a protostar grows to a size beyond 120 M, something drastic must happen. Although the limit can be stretched for very early Population III stars, and the exact value is uncertain, if any stars still exist above 150-200 M, they would challenge current theories of stellar evolution. Studying the Arches cluster, which is the densest known cluster of stars in our galaxy, astronomers have confirmed that stars in that cluster do not occur any larger than about 150 M. One theory to explain rare ultramassive stars that exceed this limit, for example in the R136 star cluster, is the collision and merger of two massive stars in a close binary system.[22]

See also[edit]


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  10. ^ Orosz, J. A.; McClintock, J. E.; Narayan, R.; Bailyn, C. D.; Hartman, J. D.; Macri, L.; Liu, J.; Pietsch, W.; Remillard, R. A.; Shporer, A.; Mazeh, T. (2007). "A 15.65-solar-mass black hole in an eclipsing binary in the nearby spiral galaxy M 33". Nature 449 (7164): 872–875. doi:10.1038/nature06218. PMID 17943124.  edit
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External links[edit]