CHAPTER III

FROM GEMINI TO LEO AND ROUND ABOUT

"If thou wouldst gaze on starry Charioteer,

And hast heard legends of the wondrous Goat,

Vast looming shalt thou find on the Twins' left,

His form bowed forward."--POSTE'S ARATUS.

[Illustration: MAP NO. 4.]

The zodiacal constellations of Gemini, Cancer, and Leo, together with

their neighbors Auriga, the Lynx, Hydra, Sextans, and Coma Berenices,

will furnish an abundance of occupation for our second night at the

telescope. We shall begin, using our three-inch glass, with alpha, the

chief star of Gemini (map No. 4). This is ordinarily known as Castor.

Even an inexperienced eye perceives at once that it is not as bright as

its neighbor Pollux, beta. Whether this fact is to be regarded as

indicating that Castor was brighter than Pollux in 1603, when Bayer

attached their Greek letters, is still an unsettled question. Castor may

or may not be a variable, but it is, at any rate, one of the most

beautiful double stars in the heavens. A power of one hundred is amply

sufficient to separate its components, whose magnitudes are about two

and three, the distance between them being 6", p. 226 deg.. A slight yet

distinct tinge of green, recalling that of the Orion nebula, gives a

peculiar appearance to this couple. Green is one of the rarest colors

among the stars. Castor belongs to the same general spectroscopic type

in which Sirius is found, but its lines of hydrogen are broader than

those seen in the spectrum of the Dog Star. There is reason for

thinking that it may be surrounded with a more extensive atmosphere of

that gaseous metal called hydrogen than any other bright star possesses.

There seems to be no doubt that the components of Castor are in

revolution around their common center of gravity, although the period is

uncertain, varying in different estimates all the way from two hundred

and fifty to one thousand years; the longer estimate is probably not far

from the truth. There is a tenth-magnitude star, distance 73", p. 164 deg.,

which may belong to the same system.

From Castor let us turn to Pollux, at the same time exchanging our

three-inch telescope for the four-inch, or, still better, the five-inch.

Pollux has five faint companions, of which we may expect to see three,

as follows: Tenth magnitude, distance 175", p. 70 deg.; nine and a half

magnitude, distance 206", p. 90 deg., and ninth magnitude, distance 229", p.

75 deg.. Burnham has seen a star of thirteen and a half magnitude, distance

43", p. 275 deg., and has divided the tenth-magnitude star into two

components, only 1.4" apart, the smaller being of the thirteenth

magnitude, and situated at the angle 128 deg.. A calculation based on Dr.

Elkin's parallax of 0.068" for Pollux shows that that star may be a

hundredfold more luminous than the sun, while its nearest companion may

be a body smaller than our planet Jupiter, but shining, of course, by

its own light. Its distance from Pollux, however, exceeds that of

Jupiter from the sun in the ratio of about one hundred and thirty to

one.

In the double star pi we shall find a good light test for our three-inch

aperture, the magnitudes being six and eleven, distance 22", p. 212 deg..

The four-inch will show that kappa is a double, magnitudes four and ten,

distance 6", p. 232 deg.. The smaller star is of a delicate blue color, and

it has been suspected of variability. That it may be variable is

rendered the more probable by the fact that in the immediate

neighborhood of kappa there are three undoubted variables, S, T, and U,

and there appears to be some mysterious law of association which causes

such stars to group themselves in certain regions. None of the variables

just named ever become visible to the naked eye, although they all

undergo great changes of brightness, sinking from the eighth or ninth

magnitude down to the thirteenth or even lower. The variable R, which

lies considerably farther west, is well worth attention because of the

remarkable change of color which it sometimes exhibits. It has been seen

blue, red, and yellow in succession. It varies from between the sixth

and seventh magnitudes to less than the thirteenth in a period of about

two hundred and forty-two days.

Not far away we find a still more curious variable zeta; this is also an

interesting triple star, its principal component being a little under

the third magnitude, while one of the companions is of the seventh

magnitude, distance 90", p. 355 deg., and the other is of the eleventh

magnitude or less, distance 65", p. 85 deg.. We should hardly expect to see

the fainter companion with the three-inch. The principal star varies

from magnitude three and seven tenths down to magnitude four and a half

in a period of a little more than ten days.

[Illustration: WONDERFUL NEBULA IN GEMINI (1532).]

With the four-or five-inch we get a very pretty sight in delta, which

appears split into a yellow and a purple star, magnitudes three and

eight, distance 7", p. 206 deg..

Near delta, toward the east, lies one of the strangest of all the

nebulae. (See the figures 1532 on the map.) Our telescopes will show it

to us only as a minute star surrounded with a nebulous atmosphere, but

its appearance with instruments of the first magnitude is so

astonishing and at the same time so beautiful that I can not refrain

from giving a brief description of it as I saw it in 1893 with the great

Lick telescope. In the center glittered the star, and spread evenly

around it was a circular nebulous disk, pale yet sparkling and

conspicuous. This disk was sharply bordered by a narrow _black_ ring,

and outside the ring the luminous haze of the nebula again appeared,

gradually fading toward the edge to invisibility. The accompanying cut,

which exaggerates the brightness of the nebula as compared with the

star, gives but a faint idea of this most singular object. If its

peculiarities were within the reach of ordinary telescopes, there are

few scenes in the heavens that would be deemed equally admirable.

In the star eta we have another long-period variable, which is also a

double star; unfortunately the companion, being of only the tenth

magnitude and distant less than 1" from its third-magnitude primary, is

beyond the reach of our telescopes. But eta points the way to one of the

finest star clusters in the sky, marked 1360 on the map. The naked eye

perceives that there is something remarkable in that place, and the

opera glass faintly reveals its distant splendors, but the telescope

fairly carries us into its presence. Its stars are innumerable, varying

from the ninth magnitude downward to the last limit of visibility, and

presenting a wonderful array of curves which are highly interesting from

the point of view of the nebular origin of such clusters. Looking

backward in time, with that theory to guide us, we can see spiral lines

of nebulous mist occupying the space that now glitters with interlacing

rows of stars. It is certainly difficult to understand how such lines of

nebula could become knotted with the nuclei of future stars, and then

gradually be absorbed into those stars; and yet, if such a process does

not occur, what is the meaning of that narrow nebulous streak in the

Pleiades along which five or six stars are strung like beads on a

string? The surroundings of this cluster, 1360, as one sweeps over them

with the telescope gradually drawing toward the nucleus, have often

reminded me of the approaches to such a city as London. Thicker and

closer the twinkling points become, until at last, as the observers eye

follows the gorgeous lines of stars trending inward, he seems to be

entering the streets of a brilliantly lighted metropolis.

Other objects in Gemini that we can ill miss are: , double, magnitudes

three and eleven, distance 73", p. 76 deg., colors yellow and blue; 15,

double, magnitudes six and eight, distance 33", p. 205 deg.; gamma,

remarkable for array of small stars near it; 38, double, magnitudes six

and eight, distance 6.5", p. 162 deg., colors yellow and blue (very pretty);

lambda, double, magnitudes four and eleven, distance 10", p. 30 deg., color

of larger star blue--try with the five-inch; epsilon, double, magnitudes

three and nine, distance 110", p. 94 deg..

From Gemini we pass to Cancer. This constellation has no large stars,

but its great cluster Praesepe (1681 on map No. 4) is easily seen as a

starry cloud with the naked eye. With the telescope it presents the most

brilliant appearance with a very low power. It was one of the first

objects that Galileo turned to when he had completed his telescope, and

he wonderingly counted its stars, of which he enumerated thirty-six, and

made a diagram showing their positions.

The most interesting star in Cancer is zeta, a celebrated triple. The

magnitudes of its components are six, seven, and seven and a half;

distances 1.14", p. 6 deg., and 5.7", p. 114 deg.. We must use our five-inch

glass in order satisfactorily to separate the two nearest stars. The

gravitational relationship of the three stars is very peculiar. The

nearest pair revolve around their common center in about fifty-eight

years, while the third star revolves with the other two, around a center

common to all three, in a period of six or seven hundred years. But the

movements of the third star are erratic, and inexplicable except upon

the hypothesis advanced by Seeliger, that there is an invisible, or

dark, star near it by whose attraction its motion is perturbed.

In endeavoring to picture the condition of things in zeta Cancri we

might imagine our sun to have a companion sun, a half or a third as

large as itself, and situated within what may be called planetary

distance, circling with it around their center of gravity; while a third

sun, smaller than the second and several times as far away, and

accompanied by a _black_ or non-luminous orb, swings with the first two

around another center of motion. There you would have an entertaining

complication for the inhabitants of a system of planets!

Other objects in Cancer are: Sigma 1223, double star, magnitudes six and

six and a half, distance 5", p. 214 deg.; Sigma 1291, double, magnitudes

both six, distance 1.3", p. 328 deg.--four-inch should split it; iota,

double, magnitudes four and a half and six and a half, distance 30", p.

308 deg.; 66, double magnitudes six and nine, distance 4.8", p. 136 deg.; Sigma

1311, double, magnitudes both about the seventh, distance 7", p. 200 deg.;

1712, star cluster, very beautiful with the five-inch glass.

[Illustration: MAP NO. 5.]

The constellation of Auriga may next command our attention (map No. 5).

The calm beauty of its leading star Capella awakens an admiration that

is not diminished by the rivalry of Orion's brilliants glittering to the

south of it. Although Capella must be an enormously greater sun than

ours, its spectrum bears so much resemblance to the solar spectrum that

a further likeness of condition is suggested. No close telescopic

companion to Capella has been discovered. A ninth-magnitude companion,

distant 159", p. 146 deg., and two others, one of twelfth magnitude at 78",

p. 317 deg., the other of thirteenth magnitude at 126", p. 183 deg., may be

distant satellites of the great star, but not planets in the ordinary

sense, since it is evident that they are self-luminous. It is a

significant fact that most of the first-magnitude stars have faint

companions which are not so distant as altogether to preclude the idea

of physical relationship.

But while Capella has no visible companion, Campbell, of the Lick

Observatory, has lately discovered that it is a conspicuous example of a

peculiar class of binary stars only detected within the closing decade

of the nineteenth century. The nature of these stars, called

spectroscopic binaries, may perhaps best be described while we turn our

attention from Capella to the second star in Auriga beta (Menkalina),

which not only belongs to the same class, but was the first to be

discovered. Neither our telescopes, nor any telescope in existence, can

directly reveal the duplicity of beta Aurigae to the eye--i. e., we can

not see the two stars composing it, because they are so close that their

light remains inextricably mingled after the highest practicable

magnifying power has been applied in the effort to separate them. But

the spectroscope shows that the star is double and that its components

are in rapid revolution around one another, completing their orbital

swing in the astonishingly short period of _four days_! The combined

mass of the two stars is estimated to be two and a half times the mass

of the sun, and the distance between them, from center to center, is

about eight million miles.

The manner in which the spectroscope revealed the existence of two

stars in beta Aurigae is a beautiful illustration of the unexpected and,

so to speak, automatic application of an old principle in the discovery

of new facts not looked for. It was noticed at the Harvard Observatory

that the lines in the photographed spectrum of beta Aurigae (and of a few

other stars to be mentioned later) appeared single in some of the

photographs and double in others. Investigation proved that the lines

were doubled at regular intervals of about two days, and that they

appeared single in the interim. The explanation was not far to seek. It

is known that all stars which are approaching us have their spectral

lines shifted, by virtue of their motion of approach, toward the violet

end of the spectrum, and that, for a similar reason, all stars which are

receding have their lines shifted toward the red end of the spectrum.

Now, suppose two stars to be revolving around one another in a plane

horizontal, or nearly so, to the line of sight. When they are at their

greatest angular distance apart as seen from the earth one of them will

evidently be approaching at the same moment that the other is receding.

The spectral lines of the first will therefore be shifted toward the

violet, and those of the second will be shifted toward the red. Then if

the stars, when at their greatest distance apart, are still so close

that the telescope can not separate them, their light will be combined

in the spectrum; but the spectral lines, being simultaneously shifted in

opposite directions, will necessarily appear to be doubled. As the

revolution of the stars continues, however, it is clear that their

motion will soon cease to be performed in the line of sight, and will

become more and more athwart that line, and as this occurs the spectral

lines will gradually assume their normal position and appear single.

This is the sequence of phenomena in beta Aurigae. And the same sequence

is found in Capella and in several other more or less conspicuous stars

in various parts of the heavens.

Such facts, like those connecting rows and groups of stars with masses

and spiral lines of nebula are obscure signboards, indicating the

opening of a way which, starting in an unexpected direction, leads deep

into the mysteries of the universe.

Southward from beta we find the star theta, which is a beautiful

quadruple. We shall do best with our five-inch here, although in a fine

condition of the atmosphere the four-inch might suffice. The primary is

of the third magnitude; the first companion is of magnitude seven and a

half, distance 2", p. 5 deg.; the second, of the tenth magnitude, distance

45", p. 292 deg.; and the third, of the tenth magnitude, distance 125", p.

350 deg..

We should look at the double Sigma 616 with one of our larger apertures

in order to determine for ourselves what the colors of the components

are. There is considerable diversity of opinion on this point. Some say

the larger star is pale red and the smaller light blue; others consider

the color of the larger star to be greenish, and some have even called

it white. The magnitudes are five and nine, distance 6", p. 350 deg..

Auriga contains several noteworthy clusters which will be found on the

map. The most beautiful of these is 1295, in which about five hundred

stars have been counted.

The position of the new star of 1892, known as Nova Aurigae, is also

indicated on the map. While this never made a brilliant appearance, it

gave rise to a greater variety of speculative theories than any previous

phenomenon of the kind. Although not recognized until January 24, 1892,

this star, as photographic records prove, was in existence on December

9, 1891. At its brightest it barely exceeded magnitude four and a half,

and its maximum occurred within ten days after its first recognition.

When discovered it was of the fifth magnitude. It was last seen in its

original form with the Lick telescope on April 26th, when it had sunk to

the lowest limit of visibility. To everybody's astonishment it

reappeared in the following August, and on the 17th of that month was

seen shining with the light of a tenth-magnitude star, _but presenting

the spectrum of a nebula!_ Its visual appearance in the great telescope

was now also that of a planetary nebula. Its spectrum during the first

period of its visibility had been carefully studied, so that the means

existed for making a spectroscopic comparison of the phenomenon in its

two phases. During the first period, when only a stellar spectrum was

noticed, remarkable shiftings of the spectral lines occurred, indicating

that two and perhaps three bodies were concerned in the production of

the light of the new star, one of which was approaching the earth, while

the other or the others receded with velocities of several hundred miles

per second! On the revival in the form of a planetary nebula, while the

character of the spectrum had entirely changed, evidences of rapid

motion in the line of sight remained.

But what was the meaning of all this? Evidently a catastrophe of some

kind had occurred out there in space. The idea of a collision involving

the transformation of the energy of motion into that of light and heat

suggests itself at once. But what were the circumstances of the

collision? Did an extinguished sun, flying blindly through space, plunge

into a vast cloud of meteoric particles, and, under the lashing impact

of so many myriads of missiles, break into superficial incandescence,

while the cosmical wrack through which it had driven remained glowing

with nebulous luminosity? Such an explanation has been offered by

Seeliger. Or was Vogel right when he suggested that Nova Aurigae could

be accounted for by supposing that a wandering dark body had run into

collision with a system of planets surrounding a decrepit sun (and

therefore it is to be hoped uninhabited), and that those planets had

been reduced to vapor and sent spinning by the encounter, the second

outburst of light being caused by an outlying planet of the system

falling a prey to the vagabond destroyer? Or some may prefer the

explanation, based on a theory of Wilsing's, that _two_ great bodies,

partially or wholly opaque and non-luminous at their surfaces, but

liquid hot within, approached one another so closely that the tremendous

strain of their tidal attraction burst their shells asunder so that

their bowels of fire gushed briefly visible, amid a blaze of spouting

vapors. And yet Lockyer thinks that there was no solid or semisolid mass

concerned in the phenomenon at all, but that what occurred was simply

the clash of two immense swarms of meteors that had crossed one

another's track.

Well, where nobody positively knows, everybody has free choice. In the

meantime, look at the spot in the sky where that little star made its

appearance and underwent its marvelous transformation, for, even if you

can see no remains of it there, you will feel your interest in the

problem it has presented, and in the whole subject of astronomy, greatly

heightened and vivified, as the visitor to the field of Waterloo becomes

a lover of history on the spot.

The remaining objects of special interest in Auriga may be briefly

mentioned: 26, triple star, magnitudes five, eight, and eleven,

distances 12", p. 268 deg., and 26", p. 113 deg.; 14, triple star, magnitudes

five, seven and a half, and eleven, distances 14", p. 224 deg., and 12.6",

p. 342 deg., the last difficult for moderate apertures; lambda, double,

magnitudes five and nine, distance 121", p. 13 deg.; epsilon, variable,

generally of third magnitude, but has been seen of only four and a half

magnitude; 41, double, magnitudes five and six, distance 8", p. 354 deg.;

996, 1067, 1119, and 1166, clusters all well worth inspection, 1119

being especially beautiful.

The inconspicuous Lynx furnishes some fine telescopic objects, all

grouped near the northwestern corner of the constellation. Without a

six-inch telescope it would be a waste of time to attack the double star

4, whose components are of sixth and eighth magnitudes, distance 0.8",

p. 103 deg.; but its neighbor, 5, a fine triple, is within our reach, the

magnitudes being six, ten, and eight, distances 30", p. 139 deg., and 96",

p. 272 deg.. In 12 Lyncis we find one of the most attractive of triple

stars, which in good seeing weather is not beyond the powers of a

three-inch glass, although we shall have a far more satisfactory view of

it with the four-inch. The components are of the sixth, seventh, and

eighth magnitudes, distances 1.4", p. 117 deg., and 8.7", p. 304 deg.. A

magnifying power which just suffices clearly to separate the disks of

the two nearer stars makes this a fine sight. A beautiful contrast of

colors belongs to the double star 14, but unfortunately the star is at

present very close, the distance between its sixth and seventh magnitude

components not exceeding 0.8", position angle 64 deg.. Sigma 958 is a pretty

double, both stars being of the sixth magnitude, distance 5", p. 257 deg..

Still finer is Sigma 1009, a double, whose stars are both a little above

the seventh magnitude and nearly equal, distance 3", p. 156 deg.. A low

power suffices to show the three stars in 19, their magnitudes being six

and a half, seven and a half, and eight, distances 15", p. 312 deg., and

215", p. 358 deg.. Webb describes the two smaller stars as plum-colored.

Plum-colored suns!

At the opposite end of the constellation are two fine doubles, Sigma

1333, magnitudes six and a half and seven, distance 1.4", p. 39 deg.; and

38, magnitudes four and seven, distance 2.9", p. 235 deg..

Under the guidance of map No. 6 we turn to Leo, which contains one of

the leading gems among the double stars, gamma, whose components, of the

second and fourth magnitudes, are respectively yellow and green, the

green star, according to some observers, having a peculiar tinge of red.

Their distance apart is 3.7", p. 118 deg., and they are undoubtedly in

revolution about a common center, the probable period being about four

hundred years. The three-inch glass should separate them easily when the

air is steady, and a pleasing sight they are.

The star iota is a closer double, and also very pretty, magnitudes four

and eight, colors lemon and light blue, distance 2.17", p. 53 deg.. Other

doubles are tau, magnitudes five and seven, distance 95", p. 170 deg.; 88,

magnitudes seven and nine, distance 15", p. 320 deg.; 90, triple, magnitudes

six, seven and a half, and ten, distance, 3.5", p. 209 deg., and 59", p.

234 deg.; 54, magnitudes four and a half and seven, distance 6.2", p. 102 deg.;

and 49, magnitudes six and nine, distance 2.4", p. 158 deg..

Leo contains a remarkable variable star, R, deep red in color, and

varying in a space of a hundred and forty-four days from the fifth to

the tenth magnitude. It has also several nebulae, of which only one needs

special mention, No. 1861. This is spindle-shaped, and large telescopes

show that it consists of three nebulae. The observer with ordinary

instruments finds little to see and little to interest him in these

small, faint nebulae.

We may just glance at two double stars in the small constellation of

Sextans, situated under Leo. These are: 9, magnitudes seven and eight,

distance 53", p. 292 deg.; and 35, magnitudes six and seven, distance 6.9",

p. 240 deg..

[Illustration: MAP NO. 6.]

Coma Berenices (map No. 6) includes several interesting objects. Let

us begin with the star 2, a double, of magnitudes six and seven and a

half, distance 3.6", p. 240 deg.. The color of the smaller star is lilac.

This hue, although not extremely uncommon among double stars elsewhere,

recurs again and again, with singular persistence, in this little

constellation. For instance, in the very next star that we look at, 12,

we find a double whose smaller component is _lilac_. The magnitudes in

12 are five and eight, distance 66", p. 168 deg.. So also the wide double

17, magnitudes five and a half and six, distance 145", exhibits a tinge

of _lilac_ in the smaller component; the triple 35, magnitudes five,

eight, and nine, distances 1", p. 77 deg., and 28.7", p. 124 deg., has four

colors yellow, _lilac_, and blue, and the double 24, magnitudes five and

six, distance 20", p. 270 deg., combines an orange with a _lilac_ star, a

very striking and beautiful contrast. We should make a mistake if we

regarded this wonderful distribution of color among the double stars as

accidental. It is manifestly expressive of their physical condition,

although we can not yet decipher its exact meaning.

The binary 42 Comae Berenicis is too close for ordinary telescopes, but

it is highly interesting as an intermediate between those pairs which

the telescope is able to separate and those--like beta Aurigae--which no

magnifying power can divide, but which reveal the fact that they are

double by the periodical splitting of their spectral lines. The orbit in

42 Comae Berenicis is a very small one, so that even when the components

are at their greatest distance apart they can not be separated by a

five-or six-inch glass. Burnham, using the Lick telescope, in 1890 made

the distance 0.7"; Hall, using the Washington telescope, in 1891 made it

a trifle more than 0.5". He had measured it in 1886 as only 0.27". The

period of revolution is believed to be about twenty-five years.

In Coma Berenices there is an outlying field of the marvelous nebulous

region of Virgo, which we may explore on some future evening. But the

nebulae in Coma are very faint, and, for an amateur, hardly worth the

trouble required to pick them up. The two clusters included in the map,

2752 and 3453, are bright enough to repay inspection with our largest

aperture.

[Illustration: MAP NO. 7.]

Although Hydra is the largest constellation in the heavens, extending

about seven hours, or 105 deg., in right ascension, it contains

comparatively few objects of interest, and most of these are in the head

or western end of the constellation, which we examined during our first

night at the telescope. In the central portion of Hydra, represented on

map No. 7, we find its leading star alpha, sometimes called Alphard, or

Cor Hydrae, a bright second-magnitude star that has been suspected of

variability. It has a decided orange tint, and is accompanied, at a

distance of 281", p. 153 deg., by a greenish tenth-magnitude star. Bu. 339

is a fine double, magnitudes eight and nine and a half, distance 1.3",

p. 216 deg.. The planetary nebula 2102 is about 1' in diameter, pale blue in

color, and worth looking at, because it is brighter than most objects of

its class. Tempel and Secchi have given wonderful descriptions of it,

both finding multitudes of stars intermingled with nebulous matter.

For a last glimpse at celestial splendors for the night, let us turn to

the rich cluster 1630, in Argo, just above the place where the stream of

the Milky Way--here bright in mid-channel and shallowing toward the

shores--separates into two or three currents before disappearing behind

the horizon. It is by no means as brilliant as some of the star clusters

we have seen, but it gains in beauty and impressiveness from the

presence of one bright star that seems to captain a host of inferior

luminaries.

Pleasures of the telescope An Illustrated Guide for Amateur Astronomers and a Popular Description of the Chief Wonders of the Heavens for General Readers · 第 3 / 10 章