Lockyer holds that these differences of spectra are due simply to

differences of temperature. According to him, the red stars, which give

the fluted spectra, are of the lowest temperature; and the temperature

of the stars of the different types gradually rises till we reach the

first type, in which the temperature is so high that the dissociation

(161) of the elements is nearly if not quite complete.

III. NEBULÆ.

Classification of Nebulæ.

370. _Planetary Nebulæ._--Many nebulæ (328) present a well-defined

circular disk, like that of a planet, and are therefore called

_planetary_ nebulæ. Specimens of planetary nebulæ are shown in Fig. 429.

[Illustration: Fig. 429.]

371. _Circular and Elliptical Nebulæ._--While many nebulæ are circular

in form, others are elliptical. The former are called _circular_ nebulæ,

and the latter _elliptical_ nebulæ. Elliptical nebulæ have been

discovered of every degree of eccentricity. Examples of various circular

and elliptical nebulæ are given in Fig. 430.

[Illustration: Fig. 430.]

372. _Annular Nebulæ._--Occasionally ring-shaped nebulæ have been

observed, sometimes with, and sometimes without, nebulous matter within

the ring. They are called _annular_ nebulæ. They are both circular and

elliptical in form. Several specimens of this class of nebulæ are given

in Fig. 431.

[Illustration: Fig. 431.]

373. _Nebulous Stars._--Sometimes one or more minute stars are enveloped

in a nebulous haze, and are hence called _nebulous stars_. Several of

these nebulæ are shown in Fig. 432.

[Illustration: Fig. 432.]

374. _Spiral Nebulæ._--Very many nebulæ disclose a more or less spiral

structure, and are known as _spiral_ nebulæ. They are illustrated in

Fig. 433. There are, however, a great variety of spiral forms. We shall

have occasion to speak of these nebulæ again (381-383).

[Illustration: Fig. 433.]

375. _Double and Multiple Nebulæ._--Many _double_ and _multiple_ nebulæ

have been observed, some of which are represented in Fig. 434.

[Illustration: Fig. 434.]

Fig. 435 shows what appears to be a double annular nebula. Fig. 436

gives two views of a double nebula. The change of position in the

components of this double nebula indicates a motion of revolution

similar to that of the components of double stars.

[Illustration: Fig. 435.]

[Illustration: Fig. 436.]

Irregular Nebulæ.

376. _Irregular Forms._--Besides the more or less regular forms of

nebulæ which have been classified as indicated above, there are many of

very irregular shapes, and some of these are the most remarkable nebulæ

in the heavens. Fig. 437 shows a curiously shaped nebula, seen by Sir

John Herschel in the southern heavens; and Fig. 438, one in _Taurus_,

known as the _Crab_ nebula.

[Illustration: Fig. 437.]

[Illustration: Fig. 438.]

377. _The Great Nebula of Andromeda._--This is one of the few nebulæ

that are visible to the naked eye. We see at a glance that it is not a

star, but a mass of diffused light. Indeed, it has sometimes been very

naturally mistaken for a comet. It was first described by Marius in

1614, who compared its light to that of a candle shining through horn.

This gives a very good idea of the impression it produces, which is that

of a translucent object illuminated by a brilliant light behind it. With

a small telescope it is easy to imagine it to be a solid like horn; but

with a large one the effect is more like fog or mist with a bright body

in its midst. Unlike most of the nebulæ, its spectrum is a continuous

one, similar to that from a heated solid, indicating that the light

emanates, not from a glowing gas, but from matter in the solid or liquid

state. This would suggest that it is really an immense star-cluster, so

distant that the highest telescopic power cannot resolve it; yet in the

largest telescopes it looks less resolvable, and more like a gas, than

in those of moderate size. If it is really a gas, and if the spectrum is

continuous throughout the whole extent of the nebula, either it must

shine by reflected light, or the gas must be subjected to a great

pressure almost to its outer limit, which is hardly possible. If the

light is reflected, we cannot determine whether it comes from a single

bright star, or a number of small ones scattered through the nebula.

With a small telescope this nebula appears elliptical, as in Fig. 439.

Fig. 440 shows it as it appeared to Bond, in the Cambridge refractor.

[Illustration: Fig. 439.]

[Illustration: Fig. 440.]

378. _The Great Nebula of Orion._--The nebula which, above all others,

has occupied the attention of astronomers, and excited the wonder of

observers, is the _great nebula of Orion_, which surrounds the middle

star of the three which form the sword of Orion. A good eye will

perceive that this star, instead of looking like a bright point, has a

hazy appearance, due to the surrounding nebula. This object was first

described by Huyghens in 1659, as follows:--

"There is one phenomenon among the fixed stars worthy of mention, which,

so far as I know, has hitherto been noticed by no one, and indeed cannot

be well observed except with large telescopes. In the sword of Orion are

three stars quite close together. In 1656, as I chanced to be viewing

the middle one of these with the telescope, instead of a single star,

twelve showed themselves (a not uncommon circumstance). Three of these

almost touched each other, and with four others shone through a nebula,

so that the space around them seemed far brighter than the rest of the

heavens, which was entirely clear, and appeared quite black; the effect

being that of an opening in the sky, through which a brighter region was

visible."

[Illustration: Fig. 441.]

The representation of this nebula in Fig. 441 is from a drawing made by

Bond. In brilliancy and variety of detail it exceeds any other nebula

visible in the northern hemisphere. In its centre are four stars, easily

distinguished by a small telescope with a magnifying power of forty or

fifty, together with two smaller ones, requiring a nine-inch telescope

to be well seen. Besides these, the whole nebula is dotted with stars.

In the winter of 1864-65 the spectrum of this nebula was examined

independently by Secchi and Huggins, who found that it consisted of

three bright lines, and hence concluded that the nebula was composed,

not of stars, but of glowing gas. The position of one of the lines was

near that of a line of nitrogen, while another seemed to coincide with a

hydrogen line. This would suggest that the nebula is a mixture of

hydrogen and nitrogen gas; but of this we cannot be certain.

[Illustration: Fig. 442.]

379. _The Nebula in Argus._--There is a nebula (Fig. 442) surrounding

the variable star _Eta Argus_ (355), which is remarkable as exhibiting

variations of brightness and of outline.

In many other nebulæ, changes have been suspected; but the

indistinctness of outline which characterizes most of these objects, and

the very different aspect they present in telescopes of different

powers, render it difficult to prove a change beyond a doubt.

380. _The Dumb-Bell Nebula._--This nebula was named from its peculiar

shape. It is a good illustration of the change in the appearance of a

nebula when viewed with different magnifying powers. Fig. 443 shows it

as it appeared in Herschel's telescope, and Fig. 444 as it appears in

the great Parsonstown reflector (20).

[Illustration: Fig. 443.]

[Illustration: Fig. 444.]

Spiral Nebulæ.

381. _The Spiral Nebula in Canes Venatici._--The great spiral nebula in

the constellation _Canes Venatici_, or the _Hunting-Dogs_, is one of the

most remarkable of its class. Fig. 445 shows this nebula as it appeared

in Herschel's telescope, and Fig. 446 shows it as it appears in the

Parsonstown reflector.

[Illustration: Fig. 445.]

[Illustration: Fig. 446.]

382. _Condensation of Nebulæ._--The appearance of the nebula just

mentioned suggests a body rotating on its axis, and undergoing

condensation at the same time.

It is now a generally received theory that nebulæ are the material out

of which stars are formed. According to this theory, the stars

originally existed as nebulæ, and all nebulæ will ultimately become

condensed into stars.

[Illustration: Fig. 447.]

[Illustration: Fig. 448.]

[Illustration: Fig. 449.]

383. _Other Spiral Nebulæ._--Fig. 447 represents a spiral nebula of the

_Great Bear_. This nebula seems to have several centres of condensation.

Fig. 448 is a view of a spiral nebula in _Cepheus_, and Fig. 449 of a

singular spiral nebula in the _Triangle_. This also appears to have

several points of condensation. Figs. 450 and 451 represent oval and

elliptical nebulæ having a spiral structure.

[Illustration: Fig. 450.]

[Illustration: Fig. 451.]

_THE MAGELLANIC CLOUDS._

[Illustration: Fig. 452.]

384. _Situation and General Appearance of the Magellanic Clouds._--The

_Magellanic clouds_ are two nebulous-looking bodies near the southern

pole of the heavens, as shown in the right-hand portion of Fig. 452. In

the appearance and brightness of their light they resemble portions of

the Milky-Way.

[Illustration: Fig. 453.]

The larger of these clouds is called the _Nubecula Major_. It is visible

to the naked eye in strong moonlight, and covers a space about two

hundred times the surface of the moon. It is shown in Fig. 453. The

smaller cloud is called the _Nubecula Minor_. It has only about a fourth

the extent of the larger cloud, and is considerably less brilliant. It

is visible to the naked eye, but it disappears in full moonlight. This

cloud is shown in Fig. 454. The region around this cloud is singularly

bare of stars; but the magnificent cluster of _Toucan_, already

described (346), is near, and is shown a little to the right of the

cloud in the figure.

[Illustration: Fig. 454.]

[Illustration: Fig. 455.]

385. _Structure of the Nubeculæ._--Fig. 455 shows the structure of these

clouds as revealed by a powerful telescope. The general ground of both

consists of large tracts and patches of nebulosity in every stage of

resolution,--from that which is irresolvable with eighteen inches of

reflecting aperture, up to perfectly separated stars, like the Milky-Way

and clustering groups. There are also nebulæ in abundance, both regular

and irregular, globular clusters in every state of condensation, and

objects of a nebulous character quite peculiar, and unlike any thing in

other regions of the heavens. In the area occupied by the _nubecula

major_ two hundred and seventy-eight nebulæ and clusters have been

enumerated, besides fifty or sixty outliers, which ought certainly to be

reckoned as its appendages, being about six and a half per square

degree; which very far exceeds the average of any other part of the

nebulous heavens. In the _nubecula minor_ the concentration of such

objects is less, though still very striking. The nubeculæ, then,

combine, each within its own area, characters which in the rest of the

heavens are no less strikingly separated; namely, those of the galactic

and the nebular system. Globular clusters (except in one region of small

extent) and nebulæ of regular elliptic forms are comparatively rare in

the Milky-Way, and are found congregated in the greatest abundance in a

part of the heavens the most remote possible from that circle; whereas

in the nubeculæ they are indiscriminately mixed with the general starry

ground, and with irregular though small nebulæ.

THE NEBULAR HYPOTHESIS.

386. _The Basis of the Nebular Hypothesis._--We have seen that the

planets all revolve around the sun from west to east in nearly the

same plane, and that the sun rotates on his axis from west to east.

The planets, so far as known, rotate on their axes from west to

east; and all the moons, except those of Uranus and Neptune, revolve

around their planets from west to east. These common features in the

motion of the sun, moons, and planets, point to the conclusion that

they are of a common origin.

387. _Kant's Hypothesis._--Kant, the celebrated German philosopher,

seems to have the best right to be regarded as the founder of the

modern nebular hypothesis. His reasoning has been concisely stated

thus: "Examining the solar system, we find two remarkable features

presented to our consideration. One is, that six planets and nine

satellites [the entire number then known] move around the sun in

circles, not only in the same direction in which the sun himself

revolves on his axis, but very nearly in the same plane. This common

feature of the motion of so many bodies could not by any reasonable

possibility have been a result of chance: we are therefore forced to

believe that it must be the result of some common cause originally

acting on all the planets.

"On the other hand, when we consider the spaces in which the planets

move, we find them entirely void, or as good as void; for, if there

is any matter in them, it is so rare as to be without effect on the

planetary motions. There is, therefore, no material connection now

existing between the planets through which they might have been

forced to take up a common direction of motion. How, then, are we to

reconcile this common motion with the absence of all material

connection? The most natural way is to suppose that there was once

some such connection, which brought about the uniformity of motion

which we observe; that the materials of which the planets are formed

once filled the whole space between them. There was no formation in

this chaos, the formation of separate bodies by the mutual

gravitation of parts of the mass being a later occurrence. But,

naturally, some parts of the mass would be more dense than others,

and would thus gather around them the rare matter which filled the

intervening spaces. The larger collections thus formed would draw

the smaller ones into them, and this process would continue until a

few round bodies had taken the place of the original chaotic mass."

Kant, however, failed to account satisfactorily for the motion of

the sun and planets. According to his system, all the bodies formed

out of the original nebulous mass should have been drawn to a common

centre so as to form one sun, instead of a system of revolving

bodies like the solar system.

388. _Herschel's Hypothesis._--The idea of the gradual transmutation

of nebulæ into stars seems to have been suggested to Herschel, not

by the study of the solar system, but by that of the nebulæ

themselves. Many of these bodies he believed to be immense masses of

phosphorescent vapor; and he conceived that these must be gradually

condensing, each around its own centre, or around the parts where it

is most dense, until it should become a star, or a cluster of stars.

On classifying the nebulæ, it seemed to him that he could see this

process going on before his eyes. There were the large, faint,

diffused nebulæ, in which the condensation had hardly begun; the

smaller but brighter ones, which had become so far condensed that

the central parts would soon begin to form into stars; yet others,

in which stars had actually begun to form; and, finally,

star-clusters in which the condensation was complete. The

spectroscopic revelations of the gaseous nature of the true nebulæ

tend to confirm the theory of Herschel, that these masses will all,

at some time, condense into stars.

389. _Laplace's Hypothesis._--Laplace was led to the nebular

hypothesis by considering the remarkable uniformity in the direction

of the rotation of the planets. Believing that this could not have

been the result of chance, he sought to investigate its cause. This,

he thought, could be nothing else than the atmosphere of the sun,

which once extended so far out as to fill all the space now occupied

by the planets. He begins with the sun, surrounded by this immense

fiery atmosphere. Since the sum total of rotary motion now seen in

the planetary system must have been there from the beginning, he

conceives the immense vaporous mass forming the sun and his

atmosphere to have had a slow rotation on its axis. As the intensely

hot mass gradually cooled, it would contract towards the centre. As

it contracted, its velocity of rotation would, by the laws of

mechanics, constantly increase; so that a time would arrive, when,

at the outer boundary of the mass, the centrifugal force due to the

rotation would counterbalance the attractive force of the central

mass. Then those outer portions would be left behind as a revolving

ring, while the next inner portions would continue to contract until

the centrifugal and attractive forces were again balanced, when a

second ring would be left behind; and so on. Thus, instead of a

continuous atmosphere, the sun would be surrounded by a series of

concentric revolving rings of vapor. As these rings cooled, their

denser materials would condense first; and thus the ring would be

composed of a mixed mass, partly solid and partly vaporous, the

quantity of solid matter constantly increasing, and that of vapor

diminishing. If the ring were perfectly uniform, this condensation

would take place equally all around it, and the ring would thus be

broken up into a group of small planets, like the asteroids. But if,

as would more likely be the case, some portions of the ring were

much denser than others, the denser portions would gradually attract

the rarer portions, until, instead of a ring, there would be a

single mass composed of a nearly solid centre, surrounded by an

immense atmosphere of fiery vapor. This condensation of the ring of

vapor around a single point would not change the amount of rotary

motion that had existed in the ring. The planet with its atmosphere

would therefore be in rotation; and would be, on a smaller scale,

like the original solar mass surrounded by its atmosphere. In the

same way that the latter formed itself first into rings, which

afterwards condensed into planets, so the planetary atmospheres, if

sufficiently extensive, would form themselves into rings, which

would condense into satellites. In the case of Saturn, however, one

of the rings was so uniform throughout, that there was no denser

portion to attract the rest around it; and thus the ring of Saturn

retained its annular form.

[Illustration: Fig. 456.]

Such is the celebrated nebular hypothesis of Laplace. It starts, not

with a purely nebulous mass, but with the sun, surrounded by an

immense atmosphere, out of which the planets were formed by gradual

condensation. Fig. 456 represents the condensing mass according to

this theory.

390. _The Modern Nebular Hypothesis._--According to the nebular

hypothesis as held at the present time, the sun, planets, and

meteoroids originated from a purely nebulous mass. This nebula first

condensed into a nebulous star, the star being the sun, and its

surrounding nebulosity being the fiery atmosphere of Laplace. The

original nebula must have been put into rotation at the beginning.

As it contracted and became condensed through the loss of heat by

radiation into space, and under the combined attraction of gravity,

cohesion, and affinity, its speed of rotation increased; and the

nebulous envelop became, by the centrifugal force, flattened into a

thin disk, which finally broke up into rings, out of which were

formed the planets and their moons. According to Laplace, the rings

which were condensed into the planets were thrown off in succession

from the equatorial region of the condensing nebula; and so the

outer planets would be the older. According to the more modern idea,

the nebulous mass was first flattened into a disk, and subsequently

broken up into rings, in such a way that there would be no marked

difference in the ages of the planets. The sun represents the

central portion of the original nebula, and the comets and

meteoroids its outlying portion. At the sun the condensation is

still going on, and the meteoroids appear to be still gradually

drawn in to the sun and planets.

The whole store of energy with which the original solar nebula was

endowed existed in it in the potential form. By the condensation and

contraction this energy was gradually transformed into the kinetic

energy of molar motion and of heat; and the heat became gradually

dissipated by radiation into space. This transformation of potential

energy into heat is still going on at the sun, the centre of the

condensing mass, by the condensation of the sun itself, and by the

impact of meteors as they fall into it.

It has been calculated, that, by the shrinking of the sun to the

density of the earth, the transformation of potential energy into

heat would generate enough heat to maintain the sun's supply, at the

present rate of dissipation, for seventeen million years. A

shrinkage of the sun which would generate all the heat he has poured

into space since the invention of the telescope could not be

detected by the most powerful instruments yet constructed.

The least velocity with which a meteoroid could strike the sun would

be two hundred and eighty miles a second; and it is easy to

calculate how much heat would be generated by the collision. It has

been shown, that, were enough meteoroids to fall into the sun to

develop its heat, they would not increase his mass appreciably

during a period of two thousand years.

The sun's heat is undoubtedly developed by contraction and the fall

of meteoroids; that is to say, by the transformation of the

potential energy of the original nebula into heat.

It must be borne in mind that the nebular hypothesis is simply a

supposition as to the way in which the present solar system may have

been developed from a nebula endowed with a motion of rotation and

with certain tendencies to condensation. Of course nothing could

have been developed out of the nebula, the germs of which had not

been originally implanted in it by the Creator.

IV. THE STRUCTURE OF THE STELLAR UNIVERSE.

391. _Sir William Herschel's View._--Sir William Herschel assumed that

the stars are distributed with tolerable uniformity throughout the space

occupied by our stellar system. He accounted for the increase in the

number of stars in the field of view as he approached the plane of the

Milky-Way, not by the supposition that the stars are really closer

together in and about this plane, but by the supposition that our

stellar system is in the form of a flat disk cloven at one side, and

with our sun near its centre. A section of this disk is shown in Fig.

457.

[Illustration: Fig. 457.]

An observer near _S_, with his telescope pointed in the direction of _S

b_, would see comparatively few stars within the field of view, because

looking through a comparatively thin stratum of stars. With his

telescope pointed in the direction _S a_, he would see many more stars

within his field of view, even though the stars were really no nearer

together, because he would be looking through a thicker stratum of

stars. As he directed his telescope more and more nearly in the

direction _S f_, he would be looking through a thicker and thicker

stratum of stars, and hence he would see a greater and greater number of

them in the field of view, though they were everywhere in the disk

distributed at uniform distances. He assumed, also, that the stars are

all tolerably uniform in size, and that certain stars appear smaller

than others, only because they are farther off. He supposed the faint

stars of the Milky-Way to be merely the most distant stars of the

stellar disk; that they are really as large as the other stars, but

appear small owing to their great distance. The disk was assumed to be

cloven on one side, to account for the division of the Milky-Way through

nearly half of its course. This theory of the structure of the stellar

universe is often referred to as the _cloven disk_ theory.

[Illustration: Fig. 458.]

392. _The Cloven Ring Theory._--According to Mädler, the stars of the

Milky-Way are entirely separated from the other stars of our system,

belonging to an outlying ring, or system of rings. To account for the

division of the Milky-Way, the ring is supposed to be cloven on one

side: hence this theory is often referred to as the _cloven ring_

theory. According to this hypothesis, the stellar system viewed from

without would present an appearance somewhat like that in Fig. 458. The

outlying ring cloven on one side would represent the stars of the

Milky-Way; and the luminous mass at the centre, the remaining stars of

the system.

The Heavens Above: A Popular Handbook of Astronomy · 第 18 / 19 段