CHAPTER II

THE RIDDLE OF THE MILKY WAY

During dark but starlit nights, the gorgeous firmament is decorated

with an irregular band of light that describes a winding path across

the heavens. It continues also in the quarters hidden from our sight so

that it may be said to surround the firmament like a girdle. This band,

which is most luminous in the Northern Hemisphere, is called “The Milky

Way.”[1] It forms an angle with the equator of about 60° and divides

the firmament in two nearly equal parts--the northern, however, is

slightly larger.

[1] The literal translation of the Swedish name is “The Wintry

Way.”

The Milky Way, no less than other stellar phenomena, attracted the

early attention of the people. The Dieri Tribe in Central Australia

says that the Milky Way is the stream of heaven and the Mexicans

consider it the source of all that is. Tradition endeavoured to explain

its origin. Its milky appearance caused the Romans to call it “_Via

Lactea_,” a name that is retained in translated form in most modern

languages. This name is coupled with the legend of the Hercules-child,

who sucked the breast of Juno and when it was pushed away by the

incensed goddess, the milk was spread across the sky.

Nevertheless, the human race, until about two hundred years ago, had

little conception of the extraordinary importance of the Milky Way.

Anaxagoras and Democritos surmised, however, that it consists of a

collection of exceedingly minute and densely clustered stars each of

which has the nature of our Sun. Ptolemy described, nearly two thousand

years ago, its position on the firmament and his observations are

valid today as far as determinations with the naked eye suffice. When

Galileo introduced the telescope, the conception of the Milky Way as

made up of innumerable stars was verified. Not quite two hundred years

ago Swedenborg, in his cosmological speculations, considered our solar

system as a part of the Galaxy. Wright, Kant, and Lambert further

amplified these theories.

The first important forward step was taken by the great William

Herschel in his statistical researches. He demonstrated that the

stars lie closer to each other the nearer the Milky Way they are

located. This is mainly true about the small stars invisible to the

naked eye while the more luminous ones are more evenly distributed

over the heavens. In certain parts of the Milky Way the stars are

over one hundred times more crowded than at its poles--that is, the

points farthest removed from the Galaxy. Herschel’s investigations

were continued and elaborated by Struve, and later by numerous other

scientists.

Through these researches, it has been determined that the Milky Way

is, so to speak, the foundation upon which the star system, visible

to us, is built. All kinds of stellar bodies have been studied and

their distribution has proved to be symmetrical with reference to the

plane of the Galaxy. The majority is greatly concentrated around the

Milky Way. To these belong the new stars which occasionally blaze into

existence, as the well-known new star in Perseus, 1901, and nearly all

of which have appeared in the Milky Way or in its immediate vicinity.

We also find there the irregular nebulæ, enormous, vastly diffused

volumes of gas, among which the best known is the Orion nebula, and

which seem to constitute the primeval matter out of which the stars are

born. We might further mention the star-clusters, dense, ball-shaped

agglomerations of stars, and the so-called planetary nebulæ, which--at

least in their visible outer shell--also consist of gas accumulations

with a spherical or ellipsoid conformation. The numerous spiral nebulæ

on the other hand, those strange stellar bodies to which we later

shall have occasion to return, are beyond comparison more frequent in

the regions surrounding the poles of the Galaxy than in the rest of the

heavens.

Many astronomers have considered the Milky Way itself a nebula. The

most common theory doubtless is that it closely conforms to a spiral

nebula--an opinion that has found a particularly warm advocate in

the Dutch astronomer, Easton (see Figure 1). A few years ago Prof.

Bohlin expressed the view that it is most akin to a planetary nebula,

or more precisely to a ring nebula which is supposed to grow out of

a planetary ellipsoid nebula by the gaseous matter being driven from

its poles toward its equator. It is of a certain interest that this

theory lends itself to the support of Swedenborg’s--nevertheless

improbable--hypothesis about the origin of the planets in the solar

system. As we later shall see the Easton conception has the better

reasons in its favour.

If classified according to age the stars are again distributed with the

Milky Way as a reference point. Thus, let us consider their evolution,

which for various reasons is assumed to take the following course.

We may commence when the star-matter existed on the nebula stage. It

then radiated the light characteristic of certain incandescent gases,

principally the lightest two, hydrogen and helium, and further of an

otherwise unknown gas called nebulium (nebula-substance). These gases

were later condensed and dark spectral lines commenced to appear

beside the bright lines of the aforesaid gases. Stars on this stage,

named after their discoverer Wolf-Rayet stars, occur only in the

immediate vicinity of the Milky Way. A later stage in their evolution

is represented by the so-called helium stars in whose spectrum the dark

helium lines preponderate. They are considerably concentrated around

our Galaxy. Somewhat more evenly distributed and yet of decidedly

greater frequence in the neighbourhood of the Milky Way, the hydrogen

stars appear, characterized by strongly developed hydrogen lines and

somewhat retreating helium lines. These stars are more developed than

the helium stars and form with them the group of white stars so named

after the colour of their light. Next in evolution follow the yellow

stars, to which our Sun belongs. Dark metal lines appear in their

spectrum. They are more evenly distributed than the groups mentioned

before. Still further is this true about the red stars whose spectra

contain the characteristic bands of chemical compounds and therefore

betray comparatively advanced cooling. They are fairly uniformly spread

over the heavens but are still somewhat more numerous in the vicinity

of the Milky Way than further therefrom.

[Illustration: Fig. 1. The Milky Way, pictured as a spiral nebula by

Easton]

These facts are demonstrated in the statistics by E. C. Pickering,

Director of the Harvard Observatory, who divided the firmament in

four equal zones, the first of which is nearest to the Milky Way (and

includes it) and the last of which contains the Galactic poles. His

table shows the percentages of different stars in each of the four

zones.

| | | _White | |

_Galactic | _Helium | _Hydrogen | Yellow | _Yellow | _Red

Latitude_ | Stars_ | Stars_ | Stars_ | Stars_ | Stars_

---------------+---------+-----------+--------+---------+-------

±8.1° | 51.2 | 37.4 | 29.7 | 29.4 | 26.7

±21.6 | 31.7 | 28.6 | 27.9 | 26.7 | 27.6

±39.8 | 11.9 | 18.3 | 21.1 | 21.9 | 23.6

±62.3 | 5.2 | 15.7 | 21.3 | 22.0 | 22.1

Number of | | | | |

stars observed | 716 | 1885 | 1329 | 1719 | 457

The difference is most pronounced in the two first groups; in the

three last it is small but unmistakable. An even distribution would

correspond to 25 per cent. in all four divisions of the heavens.

These comprehensive statistics, embracing 6106 stars, seem to indicate

that the stars in their first stage were within the Milky Way but

subsequently drifted away with increasing age. This leads us to the

thought that they originated from the irregular, nebulous accumulations

which occur in the Milky Way and in its vicinity, or more correctly

from similar formations which formerly existed in these regions but

which now have clustered into stars. This agrees very well with

another observation. With the help of the spectroscope the motion

of different stars has been determined with reference to the point

where the sun now is. The velocities have been found greater the

older the stars are as shown in the table below taken mainly from the

investigations of the renowned astronomer, Campbell.

_Mean velocity of_:

Irregular nebulæ 0 Km. ( 0 Miles) per sec.

Wolf-Rayet stars 4.5 ” ( 2.8 ” ) ” ”

Helium stars 6.5 ” ( 4.0 ” ) ” ”

Hydrogen stars 11 ” ( 6.8 ” ) ” ”

Yellow stars 15 ” ( 9.3 ” ) ” ”

Red stars 17 ” (11.5 ” ) ” ”

Planetary nebulæ 25 ” (15.5 ” ) ” ”

To these figures a few remarks founded on recent observations might be

made. The average distance between us and the stars in each group is

different and the yellow stars, to which indeed our Sun belongs, are

those nearest to us in space. They are therefore easier to observe than

stars in the other groups. Campbell’s statistics include also for this

reason a smaller number of stars in this class than in the others. It

is conceivable and by the astronomer Halm held to be true that the mean

velocity of the smaller stars is greater than that of the larger ones.

This is the condition existing in a mixture of different gas molecules,

with which the brilliant French scientist, Henri Poincaré, compared

the throng of stars, inasmuch as the heavier molecules possess the

slower motion. To confirm this W. S. Adams of the Carnegie Observatory

on Mount Wilson compared stars of equal velocity in their own orbits.

Such stars are considered to be on the average equally far removed

from us. He found the theory of Halm confirmed. The mean velocity of

the hydrogen stars was reduced from 11 km. (6.8 miles) to 7.5 km. (4.7

miles), that of the yellow stars from 15 km. (9.3 miles) to 9.2 km.

(5.8 miles), and that of the red stars from 17 km. (11.5 miles) to 14

km. (8.7 miles), while that of the helium stars remained unchanged. The

sequence of the stars arranged according to velocity in the line of

sight is evidently not modified by this new calculation.

In regard to the motion of the planetary nebulæ it should be mentioned

that Campbell in this connection has carried out a great number of new

determinations according to which the mean observed velocity of these

large bodies in the line of sight must be increased to not less than 42

km. (26 miles) per second.

Campbell and Moore contribute the following interesting data in regard

to Nebula N. G. C. 7009 (Fig. 2):

“Measures of the rotational velocity of the nebula enable us to draw

some interesting conclusions concerning its mass. On the most plausible

assumption as to the location of the axis of rotation the orbital speed

of the nebular materials lying at a distance of 9 seconds of arc from

the centre is about 6 km. (3.7 miles) per second. If we provisionally

assume the mass of the central nucleus to equal that of the Sun,

Kepler’s law connecting the periodic time with the distance from the

nucleus tells us definitely that the nebula is distant from us only 8.9

light years. This must be regarded as an improbably small value, in

view of other evidence bearing on the question. For assumed distances

of 100 and 1000 light years, which we have reason to believe are more

probable orders of nebular distance, the masses of the nebula would be

respectively 11.3 and 113 times that of the Sun, and the corresponding

periods of rotation 1371 and 13,710 years. From these considerations

it seems certain that the mass of the planetary nebula N. G. C. 7009

is several times that of the Sun. The nebula is therefore competent,

from the point of view of its mass, to develop into a system more

pretentious than is our solar system.

“A few speculations concerning this nebula may not be without interest

and value.

“The faint extensions to the east and to the west of the elliptical

figure suggest an encircling ring of materials whose principal plane,

passing through the nucleus, passes also near our (the observers’)

position in space. These extensions terminate in condensed nuclei at

equal distances from the nucleus and on exactly opposite sides of the

nucleus. The faint extensions and condensations may be and probably are

largely the effect of the edgewise projection of such a ring, as in the

case of Saturn’s rings when the observer is in the plane of the rings.

The forms of the two terminating condensations, and especially the wing

extending up and out from the east condensation, suggest that we are

not precisely in the plane of the assumed ring.

“The form of the main nebula appears to be ellipsoidal and not chiefly

elliptical.

“The space immediately surrounding the central nucleus appears to be

relatively vacuous. Aside from the nucleus, the principal mass of

visible nebulosity exists in the brilliant ring, roughly elliptical

as to its inner and outer boundaries, which occupies the region about

midway between the nucleus and the outer edge of the nebular structure.

The brilliant ring is probably in reality an ellipsoidal shell; the

projection of such a shell upon a plane at right angles to the line

of sight would naturally show a relatively dark central area, but the

projection principle may not be the only one involved.

“If this nebula is in process of development into a solar system, the

indications are for a system having certain resemblances to our solar

system. Our four outer planets have a combined mass 225 times as great

as that of the four inner planets. Similarly in N. G. C. 7009, there

is apparently a paucity of material to form planets near the nucleus

and an abundance of material for planets at greater distances from the

nucleus.”

[Illustration:

Fig. 2. Planetary nebula N.G.C. 7009 (composite drawing, from

Curtis’s photographs of the nebula made with the Crossley

reflecting telescope. The scale is in seconds of arc).

From _Proceedings of the National Academy of Sciences of U. S. A._]

Interesting observations have been presented recently also with

reference to the largest among the irregular nebulæ, namely the Orion

nebula. Three astronomers in Marseilles, Bourget, Fabry, and Buisson,

found that parts of this nebula, in the neighbourhood of the so-called

trapeze and very close to each other, moved with different velocities

and that this difference might amount to 10 km. (6.2 miles) per

second. The south-easterly part approaches us while the north-easterly

recedes from us. Consequently a violent whirl-motion undoubtedly

takes place in this region. This observation has been verified by

the well-known Chicago astronomer, Frost, who employed a different

method of investigation than his predecessors. He noted differences in

velocity amounting to 11 km. (6.8 miles) per second between points not

over two seconds of arc distant from the trapeze.

If therefore we say that the irregular nebulæ on the average possess

no motion, this statement does not preclude important local deviations

from the rule within the nebulæ, intimating a transformation which

probably leads to the concentration of the nebulous matter toward the

centre of the whirl.

Leaving out, to begin with, the planetary nebulæ, it appears that the

original matter of the stars stands still in space, that their average

velocity increases with increasing age and approaches a mean value

of about 18 km. per second or roughly 1000 times the speed of the

ordinary passenger train. Our Sun, in particular, moves with a velocity

of 20 km. (12.4 miles) per second toward a point in the constellation

Hercules 30 degrees north of the equator.

What force then shall we say it is that causes the motion of the stars?

As far as we know none but gravitation. It appears therefore as if

the gaseous primeval substance of the stars were not governed by this

force. It might prove hazardous, however, to make this assumption

as gases also possess weight and even the most rarefied strata of

the Earth’s atmosphere exert barometric pressure by virtue of their

attraction to the mass of the earth. Rather the immobility of the

nebulæ is due to the frequent collisions between the molecules in any

quantity of gas even if it be attenuated to such a high degree as in

the nebulæ. Thus, the molecules strike a balance, as it were, against

each other so that the different parts of the gas accumulations

shortly are brought to rest relative to each other. The irregular

gas mists around the Milky Way form therefore a continuous whole. A

different condition obtains in regard to condensed stellar bodies such

as the stars. They may in the densest throng move during billions of

years before they collide; but they might on the other hand enter

nebulous masses and thereby suffer gradual retardation. We now refer

to stars moving outside of the vapour clouds. They are therefore

unrestricted and the longer they have obeyed gravitation without

impeding encounters with nebulous matter, in other words the longer

the time elapsed since they emerged from the gas accumulations which

gave them birth, the swifter is their motion. Their (average) velocity

can of course not exceed a certain limit which in our parts of the

universe appears to be about 18 km. (11.2 miles) per second. Campbell’s

measurements show that for the youngest stars (all except the red) the

velocity is greatest in the plane of the Milky Way, a natural enough

condition as the attracting matter here is most abundant.

The planetary nebulæ possess a greater velocity although they, as

consisting of mist vapours, are in the first stage of evolution. Faster

yet do the spiral nebulæ move according to measurements by Wolf of

Heidelberg. This shows that they are of a different nature from the

irregular nebulæ, which form the matrix of the Milky Way. A closer

examination of the few--thirteen in all--planetary nebulæ, determined

by the American astronomer Keeler, convinced me that they approach the

Galaxy from its poles with a moderate speed, and subsequently under

the influence of its attraction curve their orbit, rapidly gain in

velocity, and finally rush into the nearest part of the Milky Way with

a very high speed.

A great number of them are no doubt caught in the mists or star-throngs

of the Milky Way after exposure to numerous collisions and sweeping

away all matter in their course. Such clean-swept traces are very

common in the area of the Milky Way. One of the most beautiful examples

is the so-called Cocoon nebula in the constellation Cygnus (the

Swan). It has left in its wake a dark rift, in whose bottom, however,

exceedingly small and evidently very remote stars are visible according

to the German astronomer Wolf (see _Worlds in the Making_, page 172,

Fig. 55).

The great mean velocity of the planetary nebulæ indicates that they

originally did not belong to the Galactic system, a conclusion also

reached by Bohlin, but for other reasons. They are nevertheless more

abundant in the neighbourhood of the Milky Way than in other parts

of the heavens. This fact, if viewed superficially, might lead to

the belief that they are indigenous to the Galactic system, but is

explained by their concentration in obedience to gravitation toward the

Milky Way.

Quite recently (1917) Van Maanen determined the distance of one of

these highly interesting celestial bodies, tabulated in the New

General Catalogue as No. 7662. Its distance was found to be only about

140 light years. This is about sixteen times the distance of Sirius and

the mean distance of a star of the fifth magnitude. This circumstance

agrees very well with the idea that this nebula is captured by the

Galactic system to which it has approached from very distant parts of

the space outside of the Galactic system.

One of the most remarkable astronomical discoveries in recent years

was made by Kapteyn, who thereby as well as by other achievements has

gained perhaps the highest rank among astronomers of today. He has

shown that the stars rushing forth in the neighbourhood of the Sun

belong to two great groups, one coming from the constellation Orion,

and the other at nearly a right angle (100°) from the constellation

Scorpio. In the former, we find nearly all the helium stars hitherto

studied. We have previously seen that these stars stand almost still

with reference to the Galaxy while the irregular nebulæ possess no

motion at all relative to the same reference point--and the Galaxy is

the natural datum-line for all astronomical measurements--so that the

motion of the first-mentioned star-group toward the Sun is principally

due to the Sun’s own motion. This group, according to Kapteyn, obeys

the law of relative star velocities even better than the combined world

of all stars; thus with reference to the Sun, the helium stars are the

slowest, the yellow stars the fastest, while the hydrogen stars occupy

a middle position, all a self-evident consequence of their own velocity

with reference to the Galaxy which increases from helium stars to

yellow stars.

Kapteyn has shown another regularity in this group which is easily

explained. We have previously mentioned that the yellow stars are most,

the helium stars least removed from their place of birth in the Milky

Way. The result is that the yellow stars appear (on the average) to

come from a point farther from the Galaxy than the apparent origin of

the hydrogen stars and more remote yet than that of the helium stars.

On account of the relatively high velocity of the yellow stars in

different directions, their stream appears to be more divergent than

the stream of hydrogen stars, and helium stars move in almost parallel

paths (nearly directly opposed to the Sun’s true motion with reference

to the Galaxy).

Similar regularities have been found by Kapteyn in the second

star-drift which would lead us to think, as indeed Kapteyn assumes,

that these stars also developed from an original nebulous mist, which

arrived in our neighbourhood from the unknown distant, but is now used

up in the formation of corresponding stars. Here again the yellow stars

should have departed farther from their matrix than the white hydrogen

stars. Helium stars are very rare in this drift, so that no reliable

statistics have as yet been made for them.

It has been one of the most difficult problems of cosmogony to form

a theory to account for the origin of the Galactic system. We may,

almost yearly, witness how new stars blaze into existence only to fade

rapidly and in a few years return to their old insignificance--that is,

they become invisible to the naked eye although through powerful lenses

we may frequently discover an exceedingly faint star in their position.

As a rule, a nebula of the planetary type is formed in the course of a

few months. Somewhat later the nebula is transformed into a Wolf-Rayet

star. It is interesting to note that Wright found the central bodies in

certain planetary nebulæ to be Wolf-Rayet stars. We have good reasons

to assume this blazing forth into light to signify the collision of two

faintly luminous or possibly extinct stars. The new lights appear also

in stellar regions where the star density is very great, particularly

in the Milky Way or its vicinity.

We see therefore repeatedly how mists with enclosed central stars

originate. They remind us to a certain extent of the Galaxy with its

clouds and stars and along the road thus suggested trials have been

made to reach the solution of the riddle. The difficulty lies in the

fact that the orbs whose collision create “new stars” are small,

probably smaller than our Sun, while the mass gathered in the Milky

Way most likely is trillions[2] of times greater than that of the Sun.

It is true that we know a few unique stars, such as Arcturus, which

exceed our Sun in size several tens of thousand times, but not even two

such stars would account for the mass of the Galaxy, and furthermore

the probability that two stellar bodies of such rare dimensions would

collide is so very small that it must be left out of account.

[2] American and French numeration; billions acc. to Swedish

and English usage.

Kapteyn’s star-drifts, containing many thousands or probably millions

of stars, appear to furnish the bridge that leads to the solution

of the riddle of the Milky Way. These drifts were once enormous

gas-clouds, in mass probably several million times greater than that

of the Sun. They also had an extension equal to trillions of stars.

The probability for the meeting of two such gas-drifts is comparatively

large and should not be much smaller than for the entrance of a

star-drift into the Milky Way, an occurrence which actually has

happened as shown by Kapteyn.

When two such enormous gas-clouds meet, each with a cosmic velocity of

about 20 km. per second, a long time would not elapse before the gas

molecules in the region of interpenetration would be retarded in their

original motions. An extraordinarily strong concentration and heating

would occur in this territory, which is surrounded by the comparatively

cold and heavy masses which remain unaffected because outside of the

impact-area. A certain degree of equalization would naturally take

place in the layers adjoining the boundary between active and inactive

parts and the former would, furthermore, be set into a rapid spin

around an axis perpendicular to the plane containing the two original

motions. On account of the great viscosity of gases, particularly

at high temperature, the central part would rotate as a coherent

unit. Thus it would form a disk of gaseous matter. This disk would be

thickest in the middle and would become thinner toward the edge where

centrifugal force acts most powerfully.

[Illustration: Fig. 3. N.G.C. 4594. Exposure = 2 hours. 1mm = 6”7.

From _Proceedings of the National Academy of Sciences of U. S. A._]

Such a discous nebula has been investigated by the astronomer F. G.

Pease of the Carnegie Observatory on Mount Wilson. By means of the

spectroscope he has studied the motion of Nebula No. 4594 in the New

General Catalogue (see Fig. 3). This body is believed to be a spiral

nebula like those in Figs. 4 and 5 but viewed from the side so that

the spirals appear as a band. As the picture shows, this band is

coursed through by a thick dark line, owing, it is believed, to a cold

non-luminous dust-cloud outside of the spiral. The bright band is

broadest in the centre. The curvature of the dark middle line in the

shape of an arc, whose apex points downward, combined with the fact

that the major portion of light falls above this arc, indicates

that we do not view the nebula exactly on edge but from the upper

(north) side of a plane through the arms of the nebula. The nucleus

speeds away from us at the dizzying rate of 1180 km. (730 miles) per

second. The east edge, _i. e._ the left on the picture, departs with

the still higher velocity of 1630 km. (1100 miles) per second, while

the west (right) edge retreats at the rate of only 800 km. (495 miles)

per second. According to Pease, the nebula rotates as a solid disk so

that the difference between the velocity of any point and that of the

centre increases in the same proportion as the distance of the point in

question from the centre. It is probable that we have been prevented

from observing the outer parts, corresponding to the spiral arms

proper, by the ring of dust which encircles the nebula. The visible

portion occupies an arc of 2¼ minutes on each side of the centre. Its

spectrum corresponds to that of star-group F-5 among the yellow stars

in the Harvard classification. Therefore, it is not the light of the

coherent gas-cloud which preponderates but rather that of the stars

consolidated within the cloud, and corresponding to the stars in the

Milky Way. This star-light is so bright that it entirely suppresses the

radiation from the gas-cloud itself.

Such parts of the gas-aggregation as are most removed from the place of

collision continue in their course through space little affected by the

attraction of the central mass because of the great distance involved.

The portions nearer the point of impact receive orbits curved by this

same attraction and the curvature becomes the sharper the nearer the

axis of rotation. One result of the mutual gravitation between the

central mass and the particles in the outer sections of the nebula is

also that the velocity in the spiral arms becomes smaller the farther

the section in question is located from the centre, just as comets in

the solar system move slower the farther they are removed from the Sun.

But in all portions outside the central region the attraction is too

weak to give circular orbits to the gaseous matter. All substance in

these localities, therefore, departs ever more from the centre. As the

spiral arms stretch out into straight lines such matter finally leaves

the central disk altogether. It is possible that only the disk itself

remains in the nebula computed by Pease.

Another astronomer on Mount Wilson, A. Van Maanen, has investigated

a nebula, No. 101 in Messier’s catalogue (Fig. 4). This nebula lies

nearly at a right angle to the line of vision which consequently almost

coincides with the axis of rotation. The motion of the different parts

of this nebula has been calculated with the help of photographs taken

in the years 1899, 1908, and 1914, whereby its changed position with

reference to surrounding fixed stars has been recorded. Out of 87

points in the spirals only 9 moved in the direction of the hands on a

clock while the other 78 moved in the opposite sense. The mean angular

velocity is 0.022 seconds of arc per year, corresponding to 85,000

years for one complete revolution at 5 minutes’ distance from the

centre. The absolute velocity 2 minutes of arc from the centre is 1.5

times as great as at 7.5 minutes’ distance.

Fig. 4 is reproduced from Van Maanen’s original. It shows clearly the

general regularity in the motion of the component parts as well as

the numerous exceptions to the rule. Such exceptions may be caused by

perturbations due to invading masses, which impart their own motion to

the entangling matter. These foreign bodies have probably condensed

surrounding vapours and this created the bright knots which stud the

nebular spirals. The upward motion amounts on the average to 0.007

seconds per year. While the points of condensation describe half a

revolution around the centre they depart therefrom to about twice their

original distance. More than a million years is therefore likely to

elapse before the outer portions of the nebula are so far removed from

the nucleus that the spiral form of the nebula is no more apparent.

[Illustration:

Fig. 4. Internal motions in Messier 101. The arrows indicate the

direction and magnitude of the mean annual motions. Their

scale (0”1) is indicated on the plate. The scale of the

nebula is 1mm = 10”5. The comparison stars are enclosed in

circles.

From _Proceedings of the National Academy of Sciences of U. S. A._]

[Illustration:

Fig. 5. Spiral nebula No. 51 in Messier’s Catalogue; situated in

Canes Venatici, and photographed February 7 and 8, 1910,

from Mount Wilson Observatory in California. Scale: 1

millimeter = 5 sec. arc.

Lyran Herkules

Ormbäraren Örnen Skölden

Svanen Räven

Pilen

Ormbäraren Skytten

Skorpionen

Södra Kronan Kolsäck

Syd-Korset

Skeppet Argo Kölen

Skeppet Argo Styre Segel

N

Enhörningen

Enhörningen

Kusken

Cepheus

Perseus

Kassiopeja

Svanen

]

It is clear that the Milky Way may have been formed through the

collision of two immense nebulous gas-aggregations in the manner just

described. Subsequently and by virtue of the magnitude of the Galaxy

great quantities of wandering cosmic matter and minor stellar bodies

have been gathered in occasionally accompanied by larger clusterings

such as the planetary nebulæ referred to.

How well justified we are in looking upon the Milky Way as a spiral

nebula is apparent from the picture (Fig. 5) reproducing a photograph

of the familiar regular nebula in the Dogs (Canes Venatici). It shows

a wealth of detail hitherto not surmised. The feat was accomplished in

the Carnegie Observatory on Mount Wilson in Southern California with

the help of optical resources vastly superior to all earlier means.

The Milky Way has previously been compared to this nebula, but due to

deficient enlargement their striking similarity has not been fully

recognized until now.

Assume the Sun located in the point marked “S” in Fig. 5 and some

distance above the plane of the picture, then the nebula if viewed

from this point would appear somewhat as the Milky Way appears to

us. In the middle we behold the substantial nucleus and on its left

side a cleft between the two branches of the inner spiral. Farther

to the left, we see only the outer spiral, first broadening toward

the left where it approaches “S,” then narrowing only to spread again

on account of the great clustering in the lower right part of the

spiral. The axis of the nebula corresponds to the densest parts of

the Galaxy in Cygnus (the Swan), the loop in the inner spiral again

to the empty space between Cepheus and Cassiopeia, the narrow part

of the outer spiral branch resembles the constriction at Algenib,

the following diffusion corresponds to the broad section in Auriga

(Charioteer) and Monoceros (Unicorn). At the subsequent narrow place

we see the outer nebula-clump corresponding in certain respects to the

Magellanic clouds on our firmament although these are farther removed,

and apparently not indigenous to the Milky Way. There follows in the

nebula a massive section in our system represented by the well known,

far less compact, yet brightly luminous tract containing the Southern

Cross. Here, from the star Alpha in Centaurus--the nearest bright fixed

star[3] to our Sun, “only” 4.5 light years or about 25 trillion[4]

miles distant--commences a bi-section of the spiral and strangely

enough the nebula is similarly forked. Now the outer spiral stretching

in a faint line upward from the “clump” begins to show as a weak band,

while the inner spiral stands forth powerfully above “S” corresponding

to the brilliant section of the Galaxy in Scutum (Shield) and Aquila

(Eagle). The partition in the nebula between these two branches is

the counterpart of the 110° long “prong” in the Milky Way between the

constellations Norma and Lyra. Numerous faint bridges join the two

branches in the nebula as well as in the Galaxy, according to Wolf.

[3] Up to a short time ago Alpha Centauri was considered the

fixed star nearest to the Sun. By comparing old photographs

of the firmament with such of recent date the renowned

astronomer Barnard found that a very small fixed star--of

the magnitude 10.5 and therefore far from visible to the

naked eye--in the constellation Ophiuchus (Right ascension

17 h. 58 m. 44 s., North declination 4° 27´.4 January 1,

1917) possesses a very large proper motion. It traverses in

a year 10.3 seconds on the firmament. The distance to this

star, which has the largest proper motion so far known,

was later determined to be 3.3 light years or 3/4 of the

distance from Alpha Centauri to our Sun. Hence its velocity

at right angle to the line of vision is computed to be

49 km. (32 miles) per second. Spectroscopic measurements

show that it approaches us with a velocity of 91 km. (56.5

miles) per second along the line of vision. The combined

velocity, therefore, is 103 km. (63 miles) per second, an

unusually high value. The value of 3.3 light years used in

this calculation was determined by the French astronomer

Gonnessiat, who found it by the study of old photographs

from Algeria. He also calculated the parallax of this star

to be 1 second. According to later measurements, given in

the Harvard Bulletins 616 and 617, its parallax is only

0.7 seconds and consequently its distance 4.6 light years

and its speed perpendicularly to the line of vision 70 km.

(43.5 miles) per second. Campbell, in the Lick Observatory,

had determined its radial velocity and found that it

approaches the Sun at the rate of 128 km. (79 miles) per

second. Its total velocity is, according to these two last

determinations, 146 km. (91 miles) per second.

It is by no means improbable that similar discoveries will

be made in the future, so that the Sun will be found to have

more stars in its “immediate” vicinity than previously

assumed.

[4] American and French numeration; the Swedish and English

usage is billion.

The correspondence is indeed surprisingly good. Proportions are, of

course, somewhat different--in particular is the central part of the

Galaxy not so predominating, which fact has been troublesome to the

adherents of the nebula theory. Probably it was originally denser but

has become attenuated through star-formation, explaining, for instance,

the great gap between the constellations Lyra and Vulpecula.

To give a better idea of the structure of the Milky Way, two

photographs are here reproduced as taken by Wolf, the German astronomer

in Heidelberg, who has done particularly meritorious work in this

department. One (Fig. 6) shows a section of the Galaxy in Cygnus

(the Swan) with the star Deneb in the centre and to the left the

“Northamerican-nebula” so named from its shape. Above Deneb is the dark

“hole” in Cygnus and below another chasm not quite so black. Left of

the “hole” is the winding canal enclosing the so-called Cocoon nebula.

(See _Worlds in the Making_, page 172.)

The following picture (Fig. 7) contains, in the upper left, the bright

star Altair in Aquila (the Eagle) located close to the powerful arm of

the Galaxy in this constellation. Farther to the right is the fainter

arm in Ophiuchus (the Serpent-holder). The lower half contains the

most brilliant part of the Milky Way in the constellations Scutum (the

Shield) and Sagittarius (the Archer). Bright stars are infrequent but

the fainter ones are innumerable: “They are crowded into dense clusters

and between them the most delicate star dust is scattered.”--“We behold

how the star-ribbon dissolves into detached tufts which intertwine into

the strangest patterns. These clouds of stars reach their greatest

splendour in the lower part of the map.”

[Illustration:

Fig. 6. The Milky Way between constellations Cassiopeia and Swan

from photo by M. Wolf of Heidelberg. A little to the left

of the middle the beautiful nebula America appears.

]

[Illustration:

Fig. 7. The Milky Way in constellations Eagle (upper half) and

Archer (lower half). In the upper left the bright star

Altair appears. Photo from M. Wolf of Heidelberg.

]

We also reproduce (Fig. 8) from M. Wolf a photograph in larger scale

from the region of Gamma (lower part of Fig. 7) in the Eagle

with its “trident-hole,” so called from its peculiar shape, and in

whose vicinity mists and star-clouds abound. This picture is a more

complicated counterpart of the flatter photograph by Wolf of the

“Cocoon nebula.” It appears as if three or four stellar bodies here

had stepped in from without, swept away the stars in their way, and

left clean “streets” behind. Probably other “empty” spots in the

neighbourhood have been formed in a similar manner. Another theory is

that such dark places are caused by opaque mist-formations which shield

the light of the stars behind from our sight.

[Illustration: Fig. 8. The trisected hole (Trifid-hole) in Eagle. Photo

from M. Wolf of Heidelberg.]

Through these pictures we gain a conception of the manner in which the

present stars in the Milky Way have clustered out of the original misty

chaos. We cannot avoid the idea of great exterior similarity between

the lumps formed in curdling or souring milk and those which we observe

in the Milky Way. The renowned French scientist Duclaux says in his

micro-biology: “In milk, commencing to sour, but yet entirely liquid,

we observe under the microscope a precipitation of tiny particles.

To begin with they are seen with difficulty and are discovered only

by slightly displacing the plane of vision. Later they develop into

distinct grains, characterized by Brownian movements, just like small

particles of clay.... Still later the phenomenon appears as a steady

molecular agglomeration. The grains have the tendency of the clay

particles to lump and precipitate.”

The first condensation-nuclei in the mist-clouds are no doubt cosmic

dust entering from without and perhaps also larger clusterings such as

meteorites and comets. At the existing low temperature, surrounding

gases condense into fluid state on the dust particles which by

virtue of these moist shells are cemented into aggregations of such

size that gravitation overcomes the repelling radiation pressure.

Gravitation assisted by the retarding vapours further mass these

aggregates together. This process of coalescence is accompanied by

heat production. Finally, small stars are formed, then groups of such

stars, while the spaces between, now comparatively devoid of matter,

appear dark much as the whey between flocks of curd. As yet, the small

stellar bodies are surrounded by quantities of dust and gas, which,

however, with continued condensation become ever more rarefied. Even

yet the big stars in Pleiades, belonging to the helium group, appear on

the photographic plates interspaced with great patches of dust-clouds.

These are now, however, so unsubstantial that they offer little

impediment to the procession of the mighty stars. The condensation

process may be greatly accelerated through the invasion of voluminous

gas nebulæ similar to the Cocoon nebula. At last all gases in the new

star condense, that is to say the shell of tenuous vapours and dust

contracts to such an insignificant thickness that it cannot be seen

except possibly from the immediate vicinity. Small bodies ingathered

through friction against the remnants of the original extended

wrapping wander as planets around the new sun, sweeping away the last

traces of unattached matter. The condensation on the new orb leaves a

“hole” in the nebulosity which in this way is transformed into stars

and their satellites which emerge from the mist and scatter on the

firmament.

The Milky Way appears to be in a rather advanced stage of this

evolution.

The “infinitely small” presents occasionally surprising likeness to the

“infinitely large.”

In this manner we can form a conception of the growth of the wonderful

structure which has brought forth the majority of the stellar bodies

that we discern. The spiral nebulæ visible at the Galactic poles are

similar formations but probably of far more modest dimensions. They may

compare to the Milky Way as the smaller planets to the Sun. According

to recent investigations the spiral nebulæ seem also to possess an

enormous velocity and they have probably invaded the Milky Way from

without.

As previously stated, an exceedingly remarkable conception of the

Milky Way exists among the Mexicans. To them it is the Matrix of all

and gave birth to the stars, the most important of which are the Sun,

the Moon, and Venus. This idea evidently agrees very well with the

results of investigations in the last few years.

Finally, a few words about the extent of the Milky Way. So far we have

not been able to measure it; only rather uncertain approximations are

possible. Wolf estimates the diameter, that is the distance between

the two spirals at the point where the Sun now is, to be about 10,000

times the distance from the Sun to the nearest fixed star, Alpha in

Centaurus, which distance on the other hand is about 10,000 times the

distance from the Sun to the remotest known planet, Neptune, or 300,000

times that from Sun to Earth. Expressed in the usual units, we arrive

at 40,000 light years or 400,000 trillion kilometres (240,000 trillion

miles). Lord Kelvin makes another estimate of 6000 light years, that is

seven times smaller. The mean diameter of the nebula proper might be

about five times larger, in round figures one hundred thousand light

years, or one billion billion kilometres (600 million billion miles).

Like a monstrous octopus, the Milky Way swims in the fathomless

ether-sea. Its dimensions are about as many times larger than those

of the earth as that globe is larger than an atom. This has caused

the gifted Irish physicist Fournier D’Albe to consider the celestial

globes as atoms, out of which systems of the order of the Milky Way

are constructed in the same manner as the earth and other stellar

bodies are upbuilt with atoms, invisible to us and yet measured with an

incredible degree of accuracy.

Fournier D’Albe goes further still. In poetic flight he does not

hesitate to endow the Milky Way organism with life. Its evolution

cannot be denied a certain similarity to the processes of life. The

great nebula owes its origin to the union of two individuals, two

nebulosities, who met in their course through boundless space. There

floated the newborn extending its tentacles in the cool ether-waves

and gained substance and strength through the smaller beings which

the surging billows brought within its reach. It has now attained

the zenith of its evolution, and is breaking up into molecules, or

solar systems, which again are composed of stellar bodies, or atoms

within the molecule. In violent exuberance of youth these rush through

space in fulfilment of their individual life. Many will in due time

undoubtedly become dust again and then serve to nourish a new youthful

nebula. Others succumb to a freezing-death but will be restored to life

in collision with a nebulosity or some other stellar body and give

form to “new stars” or planetary clouds. Again and again shall the

starry mists go through the cycle of existence and after a lifetime,

whose duration stands in proportion to their dimensions, _i. e._ may be

estimated to billions of billions of years, give rise to new celestial

beings. Thus shall it for ever continue in an eternal rhythm.

The Destinies of the Stars · 第 2 / 7 章