CHAPTER XXX.

GLOBULAR CLUSTERS.

There is no possibility of failing to recognise in a globular cluster a

true agglomeration—a structure _teres atque rotundus_. The systemic

unity of such objects is as evident as that of a “globe of dew,” though

it is by no means certain that they are not, like that “frail and fading

sphere,” in course of more or less speedy evaporation. A gradual process

of ejection is at least suggested by their streaming edges and

filamentous appendages, formed of branching rows of stars, apparently on

the move outward. One hundred and ten globular clusters were registered

by Sir John Herschel in 1864 in his “General Catalogue” of nebulæ, and

not many have since been identified. They are astonishing constructions.

Their silvery radiance is a delight to the eye; the imagination is

allured by their visionary beauty; reason is startled by the recondite

nature of the problems they intimate. What, we cannot but ask ourselves,

is the true nature of these mysterious “balls of stars”?[847] Are the

luminous particles composing them suns in the proper sense? What are

their mutual relations? How did they originate? In what are they to

eventuate? Can mechanical stability be claimed for them, or must they be

supposed to form temporary societies undermined by forces tending

towards dissolution? On all these points definite information is still

lacking; but there is no reason to despair of its future provision,

since the inclusion of globular clusters within the scope of organised

research is of quite recent date, and knowledge respecting them is

accordingly in a nascent stage.

It may, however, safely be affirmed that their components are sun-like

bodies—that they are spherical masses at an enormously high temperature,

radiating into space by means of suitably adapted photospheric

apparatus. Some are intensely actinic. They are much brighter chemically

than visually. They hence presumably emit light mainly of the shorter

wave-lengths, and are abnormally hot bodies. But the secret of their

nature cannot be divined in our present ignorance of their spectroscopic

peculiarities, and those of the individual star-points in clusters will

long remain inaccessible. Their combined light, nevertheless, where it

is concentrated into a “blaze” at the core, is capable of being

effectually analysed with powerful instruments, and the determination of

its quality is a _sine quâ non_ for progress in this branch. Until this

has been effected, there is no possibility of assigning to globular

clusters their proper place in the celestial hierarchy.

The great southern agglomerations, ω Centauri and 47 Toucani, seem

almost untouched by the wear and tear of time. They show few signs of

dilapidation. No dusky rifts, no glades or clearings are perceptible in

them; the subtraction of material (if it be going on) has made little

progress; they are as yet well compacted to the centre. Nor is a flow of

stars outward hinted at unless obscurely. They are _cleaner_ at the

edges than most objects of their class; tentacular appendages are

wanting; their components are not visibly in marching order. This may

mean that they have but newly arrived at their present state of being,

and if so, their spectra should be of an early type. To the component

stars, accordingly, a very low mean density may probably be attributed;

their attractive power will prove small relatively to their light; the

corresponding interstitial movements must be slow, and will be difficult

of detection.

[Illustration:

FIG. 47.—Photograph of ω Centauri (Bailey).

]

Just within the northern border of the Milky Way ω Centauri is visible

to the naked eye as a hazy star of the fourth magnitude.[848]

Telescopically it presents a grand aspect. Nothing more strikingly

effective can be imagined than the transformation, by optical means, of

a blurred light-spot into a glittering and multitudinous assemblage of

separate suns. Nearly 6400 can be distinguished on sensitive plates,

besides a crowd of others so small as to merge together into a grey

mottling. No true nebulosity seems to be present. The photograph from

which the counts were made by Professor and Mrs. Bailey is reproduced in

Fig. 47. It was taken at Arequipa 19th May 1893 with an exposure of two

hours in the thirteen-inch Boyden refractor. The area marked out for

investigation covered 900 square minutes. It was “fairly well filled”

with stars, and their statistical study defined the fact of their true

central crowding.[849] They condense not merely in appearance, through

the augmenting depth of spherical space in which they are distributed,

but also as a consequence of actual compression inward. The number of

stars per square minute was found, in fact, to increase in arithmetical

progression with approach to the centre. Away from it the diminution

ceased, a constant figure being reached along a line taken to be the

boundary of the cluster; and this constant, since it must represent the

areal population of the general sky, supplied a means of correcting the

apparent results for that of the cluster. Deduction was accordingly made

of 1616 unconnected stars, mere visual intruders from a limitless

background; and there remained 5050 true components, collected within a

circular space somewhat larger than that occupied by the full moon. They

average about 12·5 magnitude.

The south polar cluster, 47 Toucani, is of equal loveliness with ω

Centauri, although on a smaller scale. Its “computed diameter” is

22′[850]—that is to say, the _extra_ stars which it projects upon the

sphere die out completely at a distance of 11′ from its centre. They

number about 2300, and are distributed in accordance with the same law

noted as prevalent in the companion cluster. They are, however, even

more densely aggregated; the realm is less spacious than ω Centauri

proportionately to the throng of its inhabitants.

The great cluster in Hercules (M 13) presents a less uniform texture

than its prototypes in the southern sky. Yet its constituent orbs follow

virtually the same gradient of central compression.[851] Their

distribution is affected besides by influences of an unimaginable kind.

Three “dark lanes,” making an equiangular junction at a point south-east

of the centre, were detected with the Rosse reflector in 1850.[852] An

identical form of marking tends to recur in other parts of the cluster.

On the Lick photographs of 1890–91, Professor Holden was able to trace

no less than thirteen repetitions of it.[853] This insistence, he

remarked in a local paper, made it evident “that a definite law was

acting to produce this form, and that this law might be truly taken as

representative for this cluster. In some way there are dark lanes

produced and maintained among the hundreds of bright stars in this

globular mass, and there are _many_ such channels. How can we conceive

of such a system? It is tolerably clear that either the dark lanes are

absolutely empty of matter, or at least that they are empty of luminous

matter.” Yet neither of these alternatives seems to be in accord with

fact.

A plate exposed during ten minutes with the Crossley reflector by

Professor Keeler showed all the brighter stars in M 13.[854] Two hours

were, however, needed to bring the swarms of their faint associates into

view. In all, more than 5400 stars, fairly within the precincts of the

cluster, were counted on a negative taken 13th July 1899. A study of

their distribution, made by Mr. Palmer, Professor Keeler’s assistant,

elicited some noteworthy peculiarities.[855] The components separated,

speaking broadly, into two distinct orders of brightness, those of

intermediate magnitudes being comparatively scarce. Out of the total

number of 5482 counted on the plate, 1016 were classed as bright, 4466

as faint, or below 13·5 magnitude. Now the mode of scattering of these

two radial—they extend outward in curved rows; that of their minute

companions is more nearly globular. Moreover, the characteristic dusky

tracks are vacant only as regards the former class of objects. They are

lightly strewn with the diffusive star powder found everywhere in the

cluster. To its presence Mr. Palmer attributes the effects of nebulosity

noticed in earlier photographs. It requires a very high resolving power

to distinguish the stellar haze created by flocks and throngs of

sixteenth-magnitude stars from genuine “fluid haze”; but in this case

there seems little doubt that the feat was performed. Confirmatory

evidence of the best kind was afforded by Professor Barnard’s direct

observations with the forty-inch Yerkes refractor. They convinced him

that globular clusters are non-nebulous formations.[856] Spectrographic

impressions will probably before long add their testimony, at least in a

negative sense.

With the thirteen-inch photographic refractor of the Potsdam

Observatory, Dr. Scheiner obtained, 9th September 1891, the first plate

of M 13 on which the stars were sufficiently defined for exact

measurement.[857] He accordingly prepared a catalogue by which the

places of 833 were fixed with the utmost accuracy; and these fundamental

stars, henceforward kept under watch and ward, will perhaps one day

disclose the plan of their movements, and thus enable future astronomers

to attack, with some possibility of success, one of the most arduous

problems in celestial dynamics. It confronts them, under a still more

bewildering form, in a superb cluster in Scorpio (M 62 = N.G.C. 6266).

Here a second focus of condensation is obvious; two star-globes are

fused into one.[858] The contorted growth of a twin cherry may help us

to realise, however imperfectly, the attendant indefinite complexity of

the conflicting forces.

A compressed cluster in Serpens (M 5 = N.G.C. 5904), discovered by Kirch

in 1702, presents telescopically the appearance of a softly radiant

globe with divergent outliers. A photograph taken by Dr. Roberts 25th

April 1892, indicated a nebulous interior; but no such effect came out

on negatives exposed with Dr. Common’s five-foot reflector, nor was it

perceptible visually to Professor Barnard. It was due, presumably, to an

amalgam of faint stars forming a kind of matrix for those bright enough

to be individualised. The discovery of their variability was begun by

Mr. Packer in 1890.[859] He remarked the fluctuations of two components,

and Dr. Common suspected many more to share the same character.[860]

This premonition was followed up, though not until after five years, by

Professor Bailey’s announcement[861] that many globular clusters—say one

in five—are veritable nests of variables. Their abundance is such that

as many as a hundred—in Professor Barnard’s words—“have been found in a

space in the sky that would be covered by a pin’s-head held at the

distance of distinct vision.”[862] Of 3000 components of ω Centauri

examined within a radius of 22′, 128 were found to fluctuate to the

extent of half a magnitude or more.[863] In one case a range of five

magnitudes was observed; but that of most of the objects investigated

was limited to one and a half, or two magnitudes. Very short periods are

the rule; three are of less than seven hours; yet one is protracted to

475 days, and there will be a special interest in determining the nature

of the light-change comprised in so long a cycle. A true “Mira variable”

would seem an anomaly in a cluster made up of silvery white stars; since

we are taught by experience to associate periods of many months with

strong absorption and consequent redness of colour. But

cluster-variables belong, for the most part, to a type apart, the

character of which has been described in an earlier chapter. They have

long minima, and brief maxima attained with extraordinary rapidity. The

activity of their changes, when they set in, contrasts singularly with

the completeness of their suspension during the intervals of rest. There

is an entire absence of concert among the affected stars. Each is an

independent, self-regulated phenomenon. No more curious spectacle is

afforded by the heavens than that of a throng of seeming signal-lights

waxing and waning every few hours under the sway, obviously, of some

common law, yet with no trace of unanimity; some fading while their

neighbours are on the rise, others stationary and semi-extinct, though

only biding their time to enter upon a phase of renewed brilliancy; and

none deviating by a hair’s-breadth from the course of change

individually prescribed for it.

Eighty-five variable stars have up to the present been recognised in

Messier 5, and they agree, for the most part, quite closely in a mode of

fluctuation elucidated by Professor Bailey’s persevering inquiries.[864]

The form of their typical light-curve is not different from that

assignable to the components of ω Centauri; but they tend unmistakably

to obey a common period of approximately twelve hours, and the

oscillations of nearly all are between the fourteenth and the fifteenth

magnitudes.[865] Yet they are not executed simultaneously; a congruity

of epochs is not even distantly indicated. Professor Barnard took visual

charge in 1898 of some half a dozen of these strange objects,[866] and

his list included Packer’s original variables, Nos. 42 and 84 of the

Harvard enumeration, stars exceptional in the great assemblage of which

they form part, both as to the length of their periods and the manner of

their change. This copies the pattern set by δ Cephei; it proceeds

continuously, although not symmetrically, along a curve steep in its

upward branch, sloping gradually downward, and interrupted by a “hump,”

significant of an abortive second maximum.[867] Its time-measure is

about twenty-six days. Professor Barnard was struck with a number of

ink-black holes rending the brilliant surface of the star-globe in

Serpens. They are closely adjacent to the dense central portion, and

suggest tunnelling operations on the scale of those progressing in the

great Hercules cluster.

A cluster in Canes Venatici (M 3 = N.G.C. 5272) is similarly perforated.

Lord Rosse observed “several small dark holes” at its core, from which

“rays run out on every side.”[868] A “bifurcated dark lane” was,

moreover, perceived in the northern segment of the nuclear “blaze.” From

which we can gather that the distribution of stars in M 3 is controlled

by forces of the same nature as those ruling in M 13. Yet the two

clusters are markedly differentiated as regards light-stability. That in

Canes is already known to contain 132 variables; while in the Hercules

group diligent inquiry has failed to certify the presence of more than

two, its components actually shining much more steadily than the average

of the stellar multitude outside its limits. Eighteen hundred stars were

counted by M. Orbinsky from photographs of M 3 taken at Pulkowa in

1894,[869] and his measurement of their places will in the future supply

a test of their relative mobility.

A starry sphere in Pegasus (M 15 = N.G.C. 7078) seemed nebulous in Dr.

Roberts’s photographs;[870] but they were perhaps clouded by stellar

dust, not by true cosmical fog. Of 900 members of this collection

examined at Harvard College, 51 proved variable. The proportion in

Ihle’s great cluster in Sagittarius (M 22 = N.G.C. 4424) is much

smaller—16 to 1550; and only 10 among 600 stars tested for stability in

M 2 gave responsive signs of fluctuation. This cluster, which is

situated in Aquarius, might be the twin of that in Hercules plunged in a

deeper depth of space.[871] The clusters ω Centauri and 47 Toucani, so

much alike in other respects, deviate widely in the matter of

variability. Periodical stars by the score occur, as we have seen, in

the former stately assemblage; in the latter, only six have been

registered, notwithstanding the most careful scrutiny. Whence the

diversity? Professor Pickering[872] surmises that it depends upon the

relation of a common plane of revolution to the line of sight. Each

globular cluster would be, on this view, a system, the movements of

which, whether axial or orbital, are conducted on the same level. And

should this level happen to coincide with the visual ray, variability

would result, either through the rotation of such components as

possessed unequally luminous surfaces, or as a consequence of the

eclipses of those provided with closely revolving satellites, Yet

neither rationale of light-change can, without grave misgivings, be

admitted. Suns with dusky hemispheres, or permanently spotted, may be

treated as mathematical fictions. Nor is any evidence as yet forthcoming

that genuine eclipse-stars ever find a habitat in clusters. Certainly

none of the cluster-variables so far investigated can be accounted

such.[873] That they are rapid binaries may be plausibly surmised, but

they must be of the non-occulting sort. In eclipsing stars the maximum

is essentially permanent; the minimum is accidental. In

cluster-variables opposite conditions prevail. Habitually obscure, they

brighten incidentally.

Professor Bailey’s discovery throws open a spacious field of research.

Each variable cluster might well claim a sentinel appointed for the

exclusive following of the complex, elusive, and rapid changes which

ceaselessly develop within its compass. In December 1901, 509 components

of star-globes were reckoned as periodical. Every one of these is

perhaps a system apart; every one has its peculiarities, the inner

meaning of which can only be drawn out by sustained attention. Powerful

instruments are, moreover, required. The objects in question lie near

the limit of practicable observation; work upon them taxes modern

resources to the utmost. Nor can the photographic method alone be relied

on. Long exposures are needed to show the stars at all, and they can

naturally give no more than the “mean magnitude” during the intervals

they cover. But when these intervals bear a large proportion to the

entire period of change, such coarse-grained data cannot satisfactorily

represent the manner of its progress. The resulting light-curve, as

Professor Bailey says,[874] is always smoothed down; and it is smoothed

to the limit of a straight line, in the ultimate case of the exposure

equalling the period of a star’s variation. Hence the absolute necessity

for supplementary visual determinations to fill out the peaks and

corners rounded off by the camera. At the critical epoch, when the flash

is being turned on, every minute counts. Estimates of brightness at the

rate of ten or twelve an hour are not too numerous for the purpose of

keeping guard over the swift alterations going forward. The hourly or

two-hourly averages given on sensitive plates are wholly inadequate.

Two questions of fundamental interest present themselves in connection

with the variability of clusters. Why, we must ask, are the stars in one

globular assemblage luminously unstable, while in others, its strict

analogues, they shine quite steadily? The contrast is not explained by

any visible difference of constitution. Variability does not appear to

come in at any particular stage of growth; it is not associated with a

definite situation in the heavens; it does not characterise pierced and

outworn globes preferentially to compact ones, or _vice versâ_; it can,

in short, be correlated with no feature obvious to direct notice. It

remains to be seen whether any spectroscopic peculiarity corresponds to

it.

Again, the absence from, or extreme scarcity of Algol-stars in clusters

occasions perplexity. We are led to believe that rapid variables are, in

truth, binaries revolving in the light-period. But if so, the orbital

planes of a certain proportion of them ought to pass through the earth,

with the outcome of affording us the spectacle of so many occulting

pairs. If these do not exist, we shall be forced to conclude that

cluster-variables owe their punctuality to some other cause than the

strict time-keeping of satellites.

One of the most signal services rendered by photography to astronomy has

been in the facilities supplied by it for the measurement of

star-clusters. The relative positions, especially of the components of

compressed groups, can only with extreme difficulty be established by

direct triangulations; while every negative taken of them fixes their

configuration at a given epoch, and gives the means of determining its

changes, should they occur. Thus the places of sixty-two stars in M 5,

catalogued at Harvard College in 1897, were estimated by Professor

Pickering to be of so high a degree of accuracy that annual

displacements amounting to one-hundredth part of a second of arc can be

detected by their comparison with results similarly obtained from plates

taken a few years hence.[875] The foundations have then been laid for an

extensive superstructure of knowledge, as regards both the physical and

the dynamical condition of globular clusters; yet centuries may elapse

before it becomes possible—in Kepler’s phrase—to “think over again,”

with apprehensive minds, those wonderful “thoughts of God.”

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