Globular cluster, a large group of old stars that are closely packed in a symmetrical, somewhat spherical form. Globular clusters, so called because of their roughly spherical appearance, are the largest and most massive star clusters.
Though several globular clusters, such as Omega Centauri in the constellation Centaurus and Messier 13 (M13) in the constellation Hercules, are visible to the unaided eye as hazy patches of light, attention was paid to them only after the invention of the telescope. The first record of a globular cluster, in the constellation Sagittarius, dates to 1665 (it was later named Messier 22); the next, Omega Centauri, was recorded in 1677 by the English astronomer and mathematician Edmond Halley. Investigations of globular clusters greatly aided the understanding of the Milky Way Galaxy. In 1917, from a study of the distances and distributions of globular clusters, the American astronomer Harlow Shapley, then of the Mount Wilson Observatory in California, determined that its galactic centre lies in the Sagittarius region.
Though several globular clusters, such as Omega Centauri and Messier 13 in the constellation Hercules, are visible to the unaided eye as hazy patches of light, attention was paid to them only after the invention of the telescope. The first record of a globular cluster, in the…
The Milky Way Galaxy contains more than 150 globular clusters (the exact number is uncertain because of obscuration by dust in the Milky Way band, which probably prevents some globular clusters from being seen). They are arranged in a nearly spherical halo around the Milky Way, with relatively few toward the galactic plane, but about a third of them are concentrated around the galactic centre, as satellite systems in the rich Sagittarius-Scorpius star fields. The radial distribution, when plotted as a function of distance from the galactic centre, fits a mathematical expression of a form identical to the one describing the star distribution in elliptical galaxies, though there is an anomalous peak in the distribution at distances of about 40,000 light-years from the centre.
Globular clusters are extremely luminous objects. Their mean luminosity is the equivalent of approximately 25,000 Suns. The most luminous are 50 times brighter. The brightest stars are the red giants, bright red stars with an absolute magnitude of −2, about 600 times the Sun’s brightness, or luminosity. In relatively few globular clusters have stars as intrinsically faint as the Sun been measured, and in no such clusters have the faintest stars yet been recorded. The luminosity function for M3 shows that 90 percent of the visible light comes from stars at least twice as bright as the Sun, but more than 90 percent of the cluster mass is made up of fainter stars. The masses of globular clusters, measured by determining the dispersion in the velocities of individual stars, range from a few thousand to more than one million solar masses. The clusters are very large, with diameters measuring from 10 to as much as 300 light-years. Their apparent diameters range from one degree for Omega Centauri down to knots of one minute of arc. In a cluster such as M3, 90 percent of the light is contained within a diameter of 100 light-years, but star counts and the study of RR Lyrae member stars (whose intrinsic brightness varies regularly within well-known limits) include a larger one of 325 light-years.
Most globular clusters are highly concentrated at their centres, having stellar distributions that resemble isothermal gas spheres with a cutoff that corresponds to the tidal effects of the Galaxy. The density near the centres of globular clusters is roughly two stars per cubic light-year, compared with one star per 300 cubic light-years in the solar neighbourhood. A precise model of star distribution within a cluster can be derived from stellar dynamics, which takes into account the kinds of orbits that stars have in the cluster, encounters between these member stars, and the effects of exterior influences. The American astronomer Ivan R. King, for instance, has derived dynamical models that fit observed stellar distributions very closely. He finds that a cluster’s structure can be described in terms of two numbers: (1) the core radius, which measures the degree of concentration at the centre, and (2) the tidal radius, which measures the cutoff of star densities at the edge of the cluster. The clusters differ markedly in the degree to which stars are concentrated at their centres. Most of them appear circular and are probably spherical, but a few (e.g., Omega Centauri) are noticeably elliptical. The most elliptical cluster is M19, its major axis being about double its minor axis.
A key distinguishing feature of globular clusters in the Galaxy is their uniformly old age. Globular clusters are composed of Population II objects (i.e., old stars). Determined by comparing the stellar population of globular clusters with stellar evolutionary models, the ages of all those so far measured range from 11 billion to 13 billion years. They are the oldest objects in the Galaxy and so must have been among the first formed. That this was the case is also indicated by the fact that the globular clusters tend to have much smaller amounts of heavy elements than do the stars in the plane of the Galaxy—e.g., the Sun. Composed of stars belonging to the extreme Population II, as well as the high-latitude halo stars, these nearly spherical assemblages apparently formed before the material of the Galaxy flattened into the present thin disk. The present interstellar gas in the solar neighbourhood contains elements heavier than helium, which are called metals by astronomers, at a level of about 2 percent by mass, while the globular clusters contain as little as 0.02 percent of the same elements.
Globular clusters have been classified on the basis of increasing abundance of metals. The abundance of metals is higher for clusters near the galactic centre than for those in the halo (the outermost reaches of the Galaxy extending far above and below its plane). The amount of helium may also differ from cluster to cluster. The hydrogen in cluster stars is thought to amount to 70–75 percent by mass, helium 25–30 percent, and the heavier elements 0.01–0.1 percent. Radio astronomical studies have set a low upper limit on the amount of neutral hydrogen in globular clusters. Dark lanes of nebulous matter are puzzling features in some of these clusters. Though it is difficult to explain the presence of distinct, separate masses of unformed matter in old systems, the nebulosity cannot be foreground material between the cluster and the observer.
About 2,000 variable stars are known in the 100 or more globular clusters that have been examined. Of these, perhaps 90 percent are members of the class called RR Lyrae variables. Other variables that occur in globular clusters are Population II Cepheids, RV Tauri, and U Geminorum stars, as well as Mira stars, eclipsing binaries, and novas.
The colour of a star has been found generally to correspond to its surface temperature, and in a somewhat similar way the type of spectrum shown by a star depends on the degree of excitation of the light-radiating atoms in it and therefore also on the temperature. All stars in a given globular cluster are, within a very small percentage of the total distance, at equal distances from Earth so that the effect of distance on brightness is common to all. Colour-magnitude and spectrum-magnitude diagrams can thus be plotted for the stars of a cluster, and the position of the stars in the array, except for a factor that is the same for all stars, will be independent of distance.
In globular clusters all such arrays show a major grouping of stars along the lower main sequence, with a giant branch containing more-luminous stars curving from there upward to the red and with a horizontal branch starting about halfway up the giant branch and extending toward the blue.
This basic picture was explained as owing to differences in the courses of evolutionary change that stars with similar compositions but different masses would follow after long intervals of time. The absolute magnitude at which the brighter main-sequence stars leave the main sequence (the turnoff point, or “knee”) is a measure of the age of the cluster, assuming that most of the stars formed at the same time. Globular clusters in the Milky Way Galaxy prove to be nearly as old as the universe, averaging perhaps 14 billion years in age and ranging between approximately 12 billion and 16 billion years, although these figures continue to be revised. RR Lyrae variables, when present, lie in a special region of the colour-magnitude diagram called the RR Lyrae gap, near the blue end of the horizontal branch in the diagram.
Two features of globular cluster colour-magnitude diagrams remain enigmatic. The first is the so-called “blue straggler” problem. Blue stragglers are stars located near the lower main sequence, although their temperature and mass indicate that they already should have evolved off the main sequence, like the great majority of other such stars in the cluster. A possible explanation is that a blue straggler is the coalescence of two lower-mass stars in a “born-again” scenario that turned them into a single more-massive and seemingly younger star farther up the main sequence, although this does not fit all cases.
The other enigma is referred to as the “second parameter” problem. Apart from the obvious effect of age, the shape and extent of the various sequences in a globular cluster’s colour-magnitude diagram are governed by the abundance of metals in the chemical makeup of the cluster’s members. This is the “first parameter.” Nevertheless, there are cases in which two clusters, seemingly almost identical in age and metal abundance, show horizontal branches that are quite different: one may be short and stubby, and the other may extend far toward the blue. There is thus evidently another, as-yet-unidentified parameter involved. Stellar rotation has been mooted as a possible second parameter, but that now seems unlikely.
Integrated magnitudes (measurements of the total brightness of the cluster), cluster diameters, and the mean magnitude of the 25 brightest stars made possible the first distance determinations on the basis of the assumption that the apparent differences were due entirely to distance. The two best methods of determining a globular cluster’s distance are comparing the location of the main sequence on the colour-magnitude diagram with that of stars close to the globular cluster in the sky and using the apparent magnitudes of the globular cluster’s RR Lyrae variables. The correction factor for interstellar reddening, which is caused by the presence of intervening matter that absorbs and reddens stellar light, is substantial for many globular clusters but small for those in high galactic latitudes, away from the plane of the Milky Way. Distances range from about 7,200 light-years for M4 to an intergalactic distance of 400,000 light-years for the cluster called AM-1.
The radial velocities (the speed at which objects approach or recede from an observer, taken as positive when the distance is increasing) measured by the Doppler effect have been determined from integrated spectra for more than 140 globular clusters. The largest negative velocity is 411 km/sec (kilometres per second) for NGC 6934, while the largest positive velocity is 494 km/sec for NGC 3201. These velocities suggest that the globular clusters are moving around the galactic centre in highly elliptical orbits. The globular cluster system as a whole has a rotational velocity of about 180 km/sec relative to the Sun, or 30 km/sec on an absolute basis. For some clusters, motions of the individual stars around the massive centre have actually been observed and measured. Though proper motions of the clusters are very small, those for individual stars provide a useful criterion for cluster membership.
The two globular clusters of highest absolute luminosity are in the Southern Hemisphere in the constellations Centaurus and Tucana. Omega Centauri, with an (integrated) absolute visual magnitude of −10.26, is the richest cluster in variables, with nearly 200 known in the early 21st century. From this large group, three types of RR Lyrae stars were first distinguished in 1902. Omega Centauri is relatively nearby, at a distance of 17,000 light-years, and it lacks a sharp nucleus. The cluster designated 47 Tucanae (NGC 104), with an absolute visual magnitude of −9.42 at a similar distance of 14,700 light-years, has a different appearance, with strong central concentration. It is located near the Small Magellanic Cloud but is not connected with it. For an observer situated at the centre of this great cluster, the sky would have the brightness of twilight on Earth because of the light of the thousands of stars nearby. In the Northern Hemisphere, M13 in the constellation Hercules is the easiest to see and is the best known. At a distance of 23,000 light-years, it has been thoroughly investigated and is relatively poor in variables. M3 in Canes Venatici, 33,000 light-years away, is the cluster second richest in variables, with well more than 200 known. Investigation of these variables resulted in the placement of the RR Lyrae stars in a special region of the colour-magnitude diagram.