This is a list of the most massive stars that have been discovered, in solar mass units (M).

Uncertainties and caveats

Most of the masses listed below are contested and, being the subject of current research, remain under review and subject to constant revision of their masses and other characteristics. Indeed, many of the masses listed in the table below are inferred from theory, using difficult measurements of the stars' temperatures, composition, and absolute brightnesses. All the masses listed below are uncertain: Both the theory and the measurements are pushing the limits of current knowledge and technology. Both theories and measurements could be incorrect.

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

Complications with distance and obscuring clouds

Since massive stars are rare, astronomers must look very far from Earth to find them. All the listed stars are many thousands of light years away making their light especially faint, which makes measurements difficult. In addition to being far away, many stars of such extreme mass are surrounded by clouds of outflowing gas created by extremely powerful stellar winds. This outflow obscures the stars, making it difficult to determine the physical properties of the star needed to calculate its mass: The surrounding gas interferes with the already difficult-to-obtain measurements of stellar temperatures and brightnesses, which greatly complicates the issue of estimating internal chemical compositions and structures.

Eta Carinae is the bright spot hidden in the double-lobed dust cloud. It is the most massive star that has a Bayer designation. It was only discovered to be (at least) two stars in the past few decades.

Both the obscuring clouds and the great distances also 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 be two or more companions orbiting too closely for our telescopes to distinguish, each star possibly being massive in itself but not necessarily "supermassive" to either be on this list, or near the top of it. And certainly other combinations are possible – for example a supermassive star with one or more smaller companions or more than one giant star – but without being able to clearly see inside the surrounding cloud, it is difficult to know what kind of object is actually generating the bright point of light seen from the Earth.

More globally, statistics on stellar populations seem to indicate that the upper mass limit is in the 120-solar-mass range, so any mass estimate above this range is suspect.

Rare reliable estimates

Eclipsing binary stars are the only stars whose masses are estimated with some confidence. However, note that almost all of the masses listed in the table below were inferred by indirect methods; only a few of the masses in the table were determined using eclipsing systems.

Amongst the most reliable listed masses are those for the eclipsing binaries NGC 3603-A1, WR 21a, and WR 20a. Masses for all three were obtained from orbital measurements. This involves measuring their radial velocities and also their light curves. The radial velocities only yield minimum values for the masses, depending on inclination, but light curves of eclipsing binaries provide the missing information: inclination of the orbit to our line of sight.

Relevance of stellar evolution

Some stars may once have been more massive than they are today. Many large stars have likely suffered significant mass loss – perhaps as much as several tens of solar masses. The lost mass is expected to have been expelled by superwinds: high velocity winds that are driven by the hot photosphere into interstellar space. The process forms an enlarged extended envelope around the star that interacts with the nearby interstellar medium and infuses the adjacent volume of space with elements heavier than hydrogen or helium.

There are also – or rather were – stars that might have appeared on the list but no longer exist as stars, or are supernova impostors; today we see only their debris. The masses of the precursor stars that fueled these destructive events can be estimated from the type of explosion and the energy released, but those masses are not listed here.

This list only concerns "living" stars – those which are still seen by Earth-based observers existing as active stars: Still engaged in interior nuclear fusion that generates heat and light. That is, the light now arriving at the Earth as images of the stars listed still shows them to internally generate new energy as of the time (in the distant past) that light now being received was emitted. The list specifically excludes both white dwarfs – former stars that are now seen to be "dead" but radiating residual heat – and black holes – fragmentary remains of exploded stars which have gravitationally collapsed, even though accretion disks surrounding those black holes might generate heat or light exterior to the star's remains (now inside the black hole), radiated by infalling matter (see § Black holes below).

Mass limits

There are two related theoretical limits on how massive a star can possibly be: The accretion mass limit and the Eddington mass limit.

  • The accretion limit is related to star formation: After about 120 M have accreted in a protostar, the combined mass should have become hot enough for its heat to drive away any further incoming matter. In effect, the protostar reaches a temperature where it evaporates away material already collected as fast as it collects new material.
  • The Eddington limit is based on light pressure from the core of an already-formed star: As mass increases past ~150 M☉, the intensity of light radiated from a Population I star's core will become sufficient for the light-pressure pushing outward to exceed the gravitational force pulling inward, and the surface material of the star will be free to float away into space. Since their different compositions make them more transparent, Population II and Population III stars have higher and much higher mass limits, respectively.

Accretion limits

Astronomers have long hypothesized 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 although 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 currently the densest known cluster of stars in our galaxy, astronomers have confirmed that no stars in that cluster exceed about 150 M☉.

The R136 cluster is an unusually dense collection of young, hot, blue stars.

Rare ultramassive stars that exceed this limit – for example in the R136 star cluster – might be explained by an exceptional event hypothesized to have occurred: some of the pairs of massive stars in close orbit in young, unstable multiple-star systems must, on rare occasions, collide and merge when certain unusual circumstances hold that make a collision possible.

Eddington mass limit

Eddington's limit on stellar mass arises because of light-pressure: 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. The lowest mass for which this effect is active is the Eddington limit.

Stars of greater mass have a higher rate of core energy generation, and heavier stars' luminosities increase far out of proportion to the increase in their masses. The Eddington limit is the point beyond which a star ought to push itself apart, or at least shed enough mass to reduce its internal energy generation to a lower, sustainable rate. The actual limit-point mass depends on how opaque the gas in the star is, and metal-rich Population I stars have lower mass limits than metal-poor Population II stars. Before their demise, the hypothetical metal-free Population III stars would have had the highest allowed mass, somewhere around 300 M☉.

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 used instead.

List of the most massive known stars

Legend
Wolf–Rayet star
Luminous blue variable/Slash star
O-type star
B-type star
A-type star

The following two lists show a few of the known stars, including the stars in open clusters, OB associations, and H II regions. Despite their high luminosity, many of them are nevertheless too distant to be observed with the naked eye. Stars that are at least sometimes visible to the unaided eye have their apparent magnitude (6.5 or brighter) highlighted with a sky blue background.

The first list gives stars that are estimated to be 60 M☉ or larger; the majority of which are shown. The second list includes some notable stars which are below 60 M☉ for the purpose of comparison. The method used to determine each star's mass is included to give an idea of the data's uncertainty; note that the mass of binary stars can be determined far more accurately. The masses listed below are the stars' current (evolved) mass, not their initial (formation) mass.

Stars with 60 M☉ or greater
NameLocationM (M)L (L☉)Teff (K)Spectral typeDist. (ly)mVMass estimated byLinkRefs
R136a1R136291±467,244,000+699,000 −1,078,00046,000+1,250 −2,375WN5h163,00012.28±0.01evolution
W49-2W49 South250±1204,365,000+3,397,000 −1,910,00035,500+1,700 −1,600O2–3.5If*36,200evolution
BAT99-98NGC 20702265,012,00045,000WN6165,00013.5mass-luminosity relation
R136a2R136195±355,129,000+367,000 −342,00047,000+1,000 −625WN5h163,00012.80±0.01evolution
Melnick 42R1361893,631,00047,300O2If*163,00012.86mass-luminosity relation
R136a3R136184±405,012,000+236,000 −226,00050,000+2,500 −8,000WN5h163,00012.97±0.01evolution
W51-57G49.5-0.41601,820,000–4,786,00042,700O4V20,000evolution
HD 15558 AIC 1805≥152±51661,000O5.5III(f)24,4007.87 combinedbinary
W51-3G49.5-0.4148+105 −821,349,000+626,000 −437,000–3,890,000+4,238,000 −2,028,00039,800O3V–O8V20,000evolution
Melnick 34 AR136147±222,692,000+544,000 −453,00053,000±1,200WN5h163,00013.10 combinedmass-luminosity relation
VFTS 1022R136142.8+25.6 −25.23,020,000+782,000 −621,00042,170±1,520O3.5If*/WN7164,00013.44evolution
R136cR136142.0+32.7 −24.73,802,000+1,568,000 −1,110,00042,170±1,890WN5h163,00012.86evolution
LH 10-3209 ANGC 17631402,312,00050,900O3III(f*)160,00012.73evolution
VFTS 682Runaway from R136137.8+27.5 −15.93,236,000+838,000 −666,00054,450±1,960WN5h164,00016.08evolution
VFTS 506NGC 2070136.8±24.22,692,00055,000ON2V((n))((f*))164,00013.31evolution
Melnick 34 BR136136±202,344,000+474,000 −394,00053,000±1,200WN5h163,00013.10 combinedmass-luminosity relation
W51dG49.5-0.41351,288,000–2,884,00042,700O3V–O4V20,000evolution
NGC 3603-BHD 97950132±132,884,000+504,000 −429,00042,000±2,000WN6h24,80011.33evolution
HD 269810NGC 20291302,188,00052,500O2III(f*)163,00012.22spectroscopy
W49-1W49 cluster 1130±301,905,000+786,000 −556,00044,700+2,100 −2,000O2–3.5If*36,200evolution
R136a7R136127+15 −162,291,000+280,000 −341,00054,000+2,000 −3,000O3III(f*)163,00013.97±0.01evolution
WR 42eRunaway from HD 979501233,200,00043,700O3If*/WN625,00014.529evolution
Sk -69° 249 ANGC 20741194,130,00038,900O7If160,00012.02±0.21evolution
Sk -69° 212NGC 20441192,377,00045,400O5III(f)160,00012.416±0.0600evolution
ST5-31NGC 20741192,168,00050,700O3If*160,00012.273±0.084evolution
R136a5R136116+6 −52,089,000+149,000 −139,00048,000±750O2I(n)f*157,00013.71±0.01evolution
MSP 183Wd2115724,00049,000±3,000O3V((f))20,00013.878±0.017spectroscopy
WR 24Collinder 2281142,951,00050,100WN6ha-w14,0006.48evolution
NGC 3603-C1HD 97950113+11 −82,239,000+392,000 −333,00044,000±2,000WN6h24,80011.89 combinedevolution
Arches-F9Arches Cluster111.32,239,00036,800WN8-9h25,000wind
VFTS 545R136110.4+18.9 −16.61,995,000+516,000 −410,00047,320±1,700O2If*/WN5164,00013.40evolution
HSH95-36R136110±51,862,000+133,000 −124,00049,500+750 −1,000O2If*163,00014.41±0.01evolution
Cygnus OB2 #12 ACygnus OB21101,660,00013,700B3–4Ia+5,20011.702 combinedspectroscopy
Melnick 39 AR136109±71,585,000+654,000 −463,00044,000±2,500O3If*/WN6-A160,00013.0 combinedbinary
R136a4R136108+6 −71,905,000+90,000 −207,00050,000+500 −2,000O3V((f*))(n)157,00013.96±0.01evolution
VFTS 621NGC 20701071,380,00050,100O2V((f*))z164,00015.39mass-luminosity relation
W49-3W49 CC105±201,514,000+528,000 −392,00040,700+5,000 −4,400O3–O7V36,200evolution
R99LH 491033,162,00028,000Ofpe/WN9164,00011.520±0.049mass-luminosity relation
Arches-F6Arches Cluster101.02,089,000+255,000 −227,00033,300±1,300WN8-9ha25,000wind
Arches-F1Arches Cluster100.91,995,00033,700WN8-9h25,000wind
Peony Starnear Galactic Center1002,951,000+1,217,000 −862,00025,100WN1026,000evolution
HD 93129 AaTrumpler 14100+25 −601,413,000+172,000 −154,00052,000±3,000O2If*7,5007.310±0.011 combinedspectroscopy
Mc30-1 AMercer 30993,236,00032,200O6–7.5If+40,000evolution
VFTS 1028R136991,230,00047,300O3III(f*) or O4–5V164,00013.82mass-luminosity relation
WR 25 ATrumpler 16982,399,00050,100WN6h-w6,5008.80 combinedevolution
BI 253Runaway from R13697.6+22.2 −23.11,175,000+410,000 −304,00054,000±1,500O2V-III(n)((f*))164,00013.669±0.062evolution
R136a8R13696±61,479,000+106,000 −99,00049,500±1,250O2–3V157,00014.42±0.01evolution
W49-15W49 cluster 196±141,288,000+334,000 −265,00043,700±1,000O2–3.5If*36,200evolution
HM 1-6HM 1951,500,00044,800O5If11,00011.64evolution
NGC 3603-42HD 9795095946,00046,500O3III(f*)25,00012.86evolution
ST2-22NGC 2044941,247,00051,300O3V((f))160,00014.3evolution
VFTS 562NGC 2070941,122,00042,200O4V164,00013.66mass-luminosity relation
NGC 3603-A1aHD 9795093.3±11.01,000,00037,000O3If*/WN624,80011.18 combinedeclipsing binary
WR 21a ARunaway from Wd293.2+2.2 −1.91,514,000+224,000 −195,00042,000O2.5If*/WN6ha26,10012.661±0.03 combinedeclipsing binary
HD 303308Trumpler 16931,138,00051,300O3V9,2008.17evolution
VFTS 512NGC 2070931,096,00047,300O2V-III((f*))164,00014.28mass-luminosity relation
R136bR13692±52,239,000+160,000 −149,00035,500±750O4If163,00013.24±0.01evolution
VFTS 16Runaway from R13691.6+11.5 −10.51,318,000+341,000 −271,00050,600+500 −590O2III-If*164,00013.546±0.010evolution
NGC 346-W1NGC 346911,500,00043,400O5.5If200,00012.57evolution
NGC 3603-A3HD 9795091863,00046,400O3III(f*)24,80012.95evolution
η Carinae ATrumpler 16904,000,0009,470 (near the top of the wind)LBV7,5006.48±0.01 combinedspectroscopy
R146Runaway from R13688.4+16.9 −15.81,950,000+505,000 −401,00053,090±1,910WN5ha164,00013.116±0.0201evolution
WR 89HM 1872,138,00039,800WN8h11,00011.02±0.01evolution
Arches-F7Arches Cluster86.31,862,000+227,000 −203,00033,900±1,300WN8-9ha25,000wind
R147Runaway from R13685.6+15.2 −16.62,291,000+593,000 −471,00047,320±1,700WN5h164,00012.993±0.042evolution
Sk 80NGC 346851,500,00038,900O7If200,00012.31evolution
BAT99-92 BTarantula Nebula851,175,00023,000B1Ia165,00011.39±0.02 combinedspectroscopy
Sk -70° 91BSDL 183084.09851,00048,849ON2III165,00012.78evolution
Sk -66° 172LH 9584.09851,00048,849O2III(f*)160,00013.1evolution
Sk -68° 137Runaway from R13684.09851,00048,849O2III(f*)160,00013.346±0.0101evolution
LH 64-16NGC 200184.09851,00048849ON2III(f*)160,00013.666±0.010evolution
Melnick 33Na AR13683±191,413,000+725,000 −479,00050,000±2,500OC2.5If*163,00013.79 combinedevolution
Melnick 39 BR13683±51,000,000+413,000 −292,00048,000±2,500O3If*/WN6-A160,00013.0 combinedbinary
WR 20a AWd282.2±4.7603,000+139,000 −113,00043,000WN6ha20,00013.5 combinedeclipsing binary
Arches-F2 AArches Cluster82±121,862,000+227,000 −203,00034,100+2,000 −1,000WN8–9h25,000eclipsing binary
R139 ANGC 207081.6+7.5 −7.21,585,000+235,000 −205,00034,000±1,100O6.5I163,00011.94 combinedevolution
WR 20a BWd281.4±4.7537,000+124,000 −101,00041,840±250WN6ha20,00013.5 combinedeclipsing binary
Tr27-27Trumpler 27811,247,00037,200O8III((f))3,90013.31evolution
HSH95-46R13680+5 −61,259,000+59,000 −162,00047,500+500 −2,500O2-3III(f*)163,00014.56±0.01evolution
Arches-F15Arches Cluster79.7794,000+118,000 −102,00032,000±1,500O6–7Ia+25,000wind
BI 237BSDL 252779.66661,00051,269O2V((f*))165,00013.830±0.0431spectroscopy
VFTS 1017R13679.0+17.8 −15.91,622,000+420,000 −334,00050,120±1,800O2If*/WN5164,00014.50evolution
VFTS 151TLD1791,072,00042,200O6.5II(f)p164,000mass-luminosity relation
VFTS 94NGC 206079955,00042,200O3.5Inf*p164,00014.161±0.0271mass-luminosity relation
VFTS 1018R13679832,00042,200O3III(f*)163,00014.34mass-luminosity relation
LH 41-32NGC 191078946,00048,200O4III160,00013.086±0.0101evolution
Pismis 24-17Pismis 2478851,000O3.5III5,90011.84spectroscopy
LSS 4067HM 177794,000+118,000 −102,00040,000±2,000O4If11,00011.26±0.07evolution
W51-2G49.2-0.377+26 −22724000+167000 −136000–1288000+617000 −41700042,700+2,000 −1,900O3V–O5V20,000evolution
R139 BNGC 207076.4+7.1 −6.71,445,000+214,000 −187,00034,700±1,100O7I163,00011.94 combinedevolution
NGC 346-W3NGC 34676813,000+99,000 −88,00051,300O2III(f*)200,00012.80±0.04evolution
BAT99-68NGC 2044761,000,00045,000O3If*/WN7165,00014.13mass-luminosity relation
HD 93632Collinder 22876946,00045,400O5III(f)10,0009.10evolution
AB1DEM S10751,175,00079,000WN3ha197,00015.24±0.02spectroscopy
VFTS 457NGC 207074.6+20.1 −9.21,585,000+410,000 −326,00039,810±1,430O3.5If*/WN7164,00013.74evolution
HD 38282 ARunaway from R13674±42,754,000+336,000 −300,00050,000±2,000WN5/6h163,00011.11±0.03 combinedbinary
BAT99-6 ANGC 174774794,00045,000O3If*/WN7165,00011.95 combinedspectroscopy
VFTS 608NGC 207074724,00042,200O4III(f)164,00014.22mass-luminosity relation
HSH95-31R13673±3955,000+68,000 −64,00047,500+1,000 −750O2V((f*))163,00014.35evolution
Mc30-11Mercer 3073741,00036,800O5.5-6I-II40,000spectroscopy
Mc30-3Mercer 3073676,00039,300O6If40,000spectroscopy
VFTS 599NGC 207072.0+9.2 −7.41,023,000+265,000 −210,00047,300+820 −500O3III(f*)164,00013.80evolution
NGC 2044-W35NGC 204472863,00048,200O4III160,00014.10evolution
VFTS 542R13671.4+16.3 −11.31,445,000+374,000 −297,00044,670±2,010O2If*/WN5164,00013.47evolution
VFTS 1021R13671.4+12.7 −9.21,259,000+326,000 −259,00035,500±1,500O4If+164,00013.31evolution
ST2-1NGC 204471946,00044,100O5.5III160,00014.3evolution
NGC 3603-A1bHD 9795070.4±9.31,000,00042,000O3If*/WN524,80011.18 combinedeclipsing binary
Arches-F12Arches Cluster70.01,585,00037,300WN7–8h25,000wind
HD 37974NGC 2050701,400,00022,500B0.5Ia+163,00010.99±0.03spectroscopy
M33 X-7 BTriangulum Galaxy70.0±6.9525,000+92,000 −78,00034,000–36,000O7III–O8III2,700,00018.70binary
QZ Carinae Aa1Collinder 22869.8±5398,00029,564±1,000O9.7I9,2006.24 combinedquaternary
VFTS 125NGC 206069.6+22.3 −17.2794,000+496,000 −281,00055,150±5,520Ope164,00016.6evolution
HD 38282 BRunaway from R13669±42,455,000+300,000 −267,00045,000±2,000WN6/7h163,00011.11±0.03 combinedbinary
HD 229059Berkeley 87691,038,00026,300B1Ia3,0008.70evolution
ST2-32NGC 204469863,00045,400O5III160,00013.903±0.0921evolution
ST2-3NGC 204469863,00044,100O5.5V160,00014.264±0.1241evolution
W28-23NGC 203369655,00051,300O3V160,00013.702±0.050evolution
HD 46150NGC 224469447,000+129,000 −100,00042,500+2,100 −2,000O5V((f))z5,2006.73evolution
HD 93403 ACarina OB168.5+12.3 −14.61,047,000+49,000 −47,00039,300±1,100O5.5I10,4008.27±0.74 combinedevolution
HSH95-47R13668±4955,000+117,000 −64,00043,500+1,750 −1,000O2V((f*))163,00014.72±0.01evolution
HSH95-48R13668±4912,000+65,000 −80,00046,500+1,000 −1,500O2–3III(f*)163,00014.75±0.01evolution
HD 93130Collinder 22868863,00039,900O7II(f)10,0008.04evolution
W51-61G49.5-0.468398,000–1,259,00038,000O7.5V20,000evolution
Sk -69° 200NGC 2033671,038,00026,300B1I160,00011.18evolution
Arches-F18Arches Cluster66.91,122,00037,300O4–5Ia+25,000wind
Arches-F4Arches Cluster66.41,995,00037,300WN7–8h25,000wind
Z15Messier 8166.11,445,000+139,000 −127,00025,000±1,000B0.511,986,00020.495spectroscopy
HD 5980 BNGC 34666±101,778,000+734,000 −519,00045,000+10,000 −7,000WN6−7200,00011.31±0.08 combinedbinary
Sk -67° 108LMC66±2933,000+67,000 −82,00043,500+750 −1,000O5III(f)164,00012.525evolution
HD 190429 Anear Barnard 14666.0+17.4 −13.4912,00039,000O4If7,8007.09±0.01spectroscopy
LH 31-1003NGC 185866863,00041,900O6Ib(f)160,00013.186±0.0101evolution
VFTS 169NGC 206066.0±9.8813,000+284,000 −210,00047,000±1,500O2.5V(n)((f*))164,00014.437±0.0251evolution
Pismis 24-1SWPismis 2466646,000O4III6,500evolution
HSH95-89R13665+10 −9977,000+198,000 −145,00044,000±2,500O4V163,00014.76±0.01spectroscopy
HSH95-40R13665+6 −7851,000+104,000 −159,00047,500+2,000 −3,250O3V163,00014.49evolution
HSH95-58R13665+6 −7741,000+150,000 −96,00047,500+3,000 −2,250O2–3V163,00014.80±0.01evolution
VFTS 145TLD165741,00039,800O8fp164,00014.30mass-luminosity relation
VFTS 518NGC 207065562,00044,700O3.5III(f*)164,00015.11mass-luminosity relation
W49-8W49 CC65±13676,000+279,000 −197,00040,700+5,000 −4,400O3–O7V36,200evolution
BD+43° 3654Runaway from Cygnus OB264.62,030,000±210,00046,800±900O6If+5,40010.06±0.04evolution
Sk -70° 115NGC 212264+3 −21,047,000+101,000 −92,00034,750±1,000O6.5Ifc164,00012.166±0.0900evolution
Sk -69° 25NGC 174864787,00043,600O6V((f))160,00011.886±0.0101evolution
HSH95-50R13664+5 −4708,000+86,000 −62,00047,000+2,000 −1,250O3–4V((f*))163,00014.65±0.01evolution
W49-5W49 cluster 164±8661,000+171,000 −136,00042,700+2,000 −1,900O3–O5V36,200evolution
ST5-71NGC 207463718,00045,400O5III160,00013.266±0.0201evolution
VFTS 259Tarantula Nebula62.6+7.8 −8.61,000,000+259,000 −206,00036,800+500 −520O6Iaf164,00013.65evolution
Mc30-6a AMercer 30621,349,00029,900Ofpe/WN940,000evolution
AB9DEM S80621,122,000100,000WN3ha197,00015.26±0.13spectroscopy
LH 41-1017NGC 191062787,00042,700B1160,00012.266±0.0101evolution
Brey 32 BNGC 196662718,00043,600O6.5V165,00012.317±0.02 combinedevolution
HD 93160Trumpler 1462718,00042,700O6III8,0007.60evolution
HSH95-35R13662+4 −3661,000+64,000 −44,00047,500+1,500 −1,000O3V163,00014.32±0.01evolution
HD 229196Cygnus OB961.640,862O55,0008.59evolution
HD 5980 ANGC 34661±102,239,000+580,000 −460,00045,000±5,000WN6h200,00011.31±0.08 combinedbinary
WR 102hbQuintuplet cluster612,630,00025,100WN9h26,000evolution
VFTS 267Tarantula Nebula61+3 −2813,000+78,000 −72,00042,500±1,250O3.5III(f*)164,00013.49evolution
LH 41-18NGC 191061787,00038,500O8.5V((f))160,00012.586±0.0101evolution
AB8 BNGC 602c61+14 −25708,000+183,000 −146,00045,000±5,000O4V197,00012.90 combinedbinary
Mc30-9 AMercer 3061676,00034,500O6-7I-III40,000evolution
ST5-25NGC 207461545,00048,600O4V160,00013.551±0.109spectroscopy
VFTS 422NGC 207061501,00039,800O4III(f)164,00015.14mass-luminosity relation
Sk -67° 166NGC 201460.68832,00041,809O4If+160,00012.22±0.03spectroscopy
Sk -65° 47NGC 192360.68832,00041,809O4If160,00012.466±0.1521spectroscopy
Mc30-7 AMercer 30601,738,00041,400WN640,000evolution
BAT99-96NGC 207060.0+9.2 −7.71,349,000+349,000 −277,00041,690±1,500WN8(h)164,00013.76evolution
Arches-F2 BArches Cluster60±81,349,000+165,000 −147,00033,800+2,000 −1,000O5–6Ia+25,000eclipsing binary
HSH95-55R13660+6 −5589,000+119,000 −52,00047,500+3,000 −1,500O2V((f*))z163,00014.74±0.01evolution

A few notable large stars with masses less than 60 M☉ are shown in the table below for the purpose of comparison, ending with the Sun, which is very close, but would otherwise be too small to be included in the list. At present, all the listed stars are naked-eye visible and relatively nearby.

Star nameLocationMass(M, Sun = 1)Eff. temp.(K)Approx. dist. (ly)Appt. vis. mag.Mass est. methodLinkRef.
λ CepheiRunaway star from Cepheus OB351.436,0003,1005.05spectroscopy
τ Canis Majoris AaNGC 23625032,0005,1204.89evolution
θ Muscae AbCentaurus OB14433,0007,4005.53 combinedevolution
θ2 Orionis AOrion OB1 of Orion complex3934,9001,5005.02evolution
α CamelopardalisRunaway star from NGC 150237.629,0006,0004.29evolution
P CygniIC 4996 of Cygnus OB13718,7005,1004.82spectroscopy
ζ1 ScorpiiNGC 6231 of Scorpius OB136 - 5317,2008,2104.705spectroscopy
ζ Orionis AaAlnitak in Orion OB1 of Orion complex3329,5001,2602.08evolution
θ1 Orionis C1Trapezium Cluster of Orion complex3339,0001,3405.13 combinedevolution
κ CassiopeiaeCassiopeia OB143323,5004,0004.16evolution
μ NormaeNGC 61693328,0003,2604.91spectroscopy
η Carinae BTrumpler 16 of Carina Nebula3037,2007,5004.3 combinedbinary
γ2 Velorum BVela OB228.535,0001,2301.83 combinedevolution
Alnilamε Orionis in Orion OB1 of Orion complex28.4±2.025,0001,2501.69spectroscopy + interferometry
Meissa AIn Collinder 69 of Orion complex27.937,7001,3003.54spectroscopy
ξ PerseiMenkib in California Nebula of Perseus OB226.135,0001,2004.04evolution
ζ PuppisNaos in Vela R2 of Vela Molecular Ridge25.3±5.340,0001,0802.25empirical
WR 79aNGC 6231 of Scorpius OB124.435,0005,6005.77spectroscopy
Mintaka Aa1In Orion OB1 of Orion complex2429,5001,2002.5 combinedevolution
ι Orionis Aa1Hatysa in NGC 1980 of Orion complex23.132,5001,3402.77 combinedevolution
κ CrucisJewel Box Cluster of Centaurus OB12316,3007,5005.98evolution
WR 78NGC 6231 of Scorpius OB12250,1004,1006.48spectroscopy
ο2 Canis MajorisField star21.415,5002,8003.043evolution
Rigel AIn Orion OB1 of Orion complex2112,1008600.13evolution
ζ OphiuchiUpper Scorpius subgroup of Scorpius OB220.234,0003702.569evolution
υ OrionisOrion OB1 of Orion complex2033,4002,9004.618evolution
σ Orionis AaOrion OB1 of Orion complex1835,0001,2604.07 combinedspectroscopy
μ ColumbaeRunaway star from Trapezium Cluster1633,0001,3005.18spectroscopy
SaiphIn Orion OB1 of Orion complex15.526,5006502.09evolution
σ CygniCygnus OB41510,8003,2604.233evolution
θ Carinae AIC 2602 of Scorpius OB214.931,0004602.76 combinedevolution
θ2 Orionis BOrion OB1 of Orion complex14.829,3001,5006.38spectroscopy
ζ PerseiPerseus OB214.520,8007502.86evolution
σ Orionis BOrion OB1 of Orion complex1431,0001,2604.07 combinedspectroscopy
β Canis MajorisMirzam in Local Bubble of Scorpius OB213.523,2004901.985evolution
ε Persei Aα Persei Cluster13.526,5006402.88 combinedevolution
ι Orionis Aa2NGC 1980 of Orion complex13.127,0001,3402.77 combinedevolution
δ Scorpii ADschubba in Upper Scorpius subgroup of Scorpius OB21327,4004402.307 combinedevolution
σ Orionis AbOrion OB1 of Orion complex1329,0001,2604.07 combinedspectroscopy
θ Muscae AaWR 48 in Centaurus OB111.583,0007,4005.53 combinedspectroscopy
γ2 Velorum AWR 11 in Vela OB2957,0001,2301.83 combinedspectroscopy
ρ Ophiuchi Aρ Ophiuchi cloud complex of Scorpius OB28.722,0003604.63 combinedevolution
BellatrixIn Bellatrix Cluster of Orion complex7.721,8002501.64evolution
Antares BLoop I Bubble of Scorpius OB27.218,5005505.5evolution
λ Tauri APisces-Eridanus stellar stream7.1818,7004803.47 combinedevolution
δ Perseiα Persei Cluster714,9005203.01evolution
ψ Perseiα Persei Cluster6.216,0005804.31evolution
α Pavonis AaPeacock in Tucana-Horologium association5.9117,7001801.94evolution
AlcyoneIn Pleiades5.912,3004402.87 combinedevolution
γ Canis MajorisMuliphein in Collinder 1215.613,6004404.1evolution
η Canis MajorisAludra in Collinder 1215.5 or 9.515,0002,0002.45SED modelling / spectroscopy
ο VelorumIC 2391 of Scorpius OB25.516,2004903.6evolution
ο AquariiPisces-Eridanus stellar stream4.213,5004404.71evolution
ν FornacisPisces-Eridanus stellar stream3.6513,4003704.69evolution
φ EridaniTucana-Horologium association3.5513,7001503.55evolution
η Chamaeleontisη Chamaeleontis moving group of Scorpius OB23.212,5003105.453evolution
ε Chamaeleontisε Chamaeleontis moving group of Scorpius OB22.8710,9003604.91evolution
τ1 AquariiPisces-Eridanus stellar stream2.6810,6003205.66evolution
ε HydriTucana-Horologium association2.6411,0001504.12evolution
β1 TucanaeTucana-Horologium association2.510,6001404.37evolution
Sirius A~11 th nearest star2.069,8508.6−1.46evolution
SunSolar System15,7720.0000158−26.744standard

Black holes

Black holes are the end point of the evolution of massive stars. Technically they are not stars, as they no longer generate heat and light via nuclear fusion in their cores. Some black holes may have cosmological origins, and would then never have been stars. This is thought to be especially likely in the cases of the most massive black holes.

See also

Footnotes

External links

  • . HubbleSite. May 2005.
  • . Space.com. 7 June 2007.
  • . ScienceDaily. March 2005.
  • . 3towers. Archived from on 2007-10-28.
  • . NASA. March 2016.