This shows the earth and the moon in their relative sizes; while

the diagram below it illustrates the distance apart.

]

[Sidenote: Laplace’s Theory Abandoned]

A fundamental difficulty is the extreme tenuity of the gas which is

assumed to have formed the planetary rings. A second difficulty, which

has been emphasised by Professors Chamberlin and Moulton, is to be

found in the comparatively small amount of rotational energy which

the system at present possesses, for this is less than 1/200 of that

which, on the most favourable assumption, must have been contained

within the original nebula. Less fundamental, but equally fatal, is the

fact that one of the satellites of Saturn revolves round its primary

in a direction opposed to that of the rotation of the planet itself.

[Recently Mr. Stratton, following out a suggestion of Professor W. H.

Pickering, has shown that this is quite consistent, and, indeed, is a

natural deduction from Laplace’s hypothesis.] Hence for these and other

reasons we are reluctantly compelled to abandon an hypothesis which

for over a century has exercised an influence on our conception of the

cosmos not less profound, penetrating, and far-reaching than that of

the famous Darwinian doctrine of natural selection, now on its trial.

[Sidenote: What are the Nebulæ?]

At present, unanimity of opinion, even on questions of the most primary

kind, is far to seek. Philosophers are not even agreed as to the

constitution of the nebulæ. It is questioned whether even those least

resolvable and most diffused forms which give bright line spectra

really consist of masses of incandescent gas. Many observers, among

them Sir Norman Lockyer, now maintain that they are formed of swarms of

meteorites, which, moving with prodigious velocity, meet in frequent

collision, and by their impact evolve sufficient heat to become

self-luminous. Others, again, like the distinguished investigator

Arrhenius, while admitting the gaseous nature of these nebulæ, deny

that they are incandescent, and assert that their temperature is not

much above that of surrounding space. Their exterior parts consist of

the lighter gases in a highly rarefied state, and minute particles of

negative electricity, which are always careering through space, on

penetrating these gases produce a luminous discharge. A nebula composed

of swarms of meteorites would, as Sir George Darwin has shown, behave

very much in the same way as one composed of gas, and if in rotation

would rotate as a solid mass. The meteorites would stand in the same

relation to the nebula as molecules to a gas, and thus the question of

the constitution of the nebula, although of great interest in itself,

becomes of subsidiary importance in tracing its subsequent history.

[Sidenote: Shaping of the Planets]

One of the latest attempts to frame a nebular hypothesis is that of

Professor J. H. Jeans. His reasoning is of a highly mathematical

character, and his conclusions are expressed in the most general terms.

Starting with a spherical nebula of gas or meteorites endowed with a

small amount of rotation, he shows that as it cools or loses energy

the temperature of the interior will not fall continuously in precise

correspondence with the cooling of the outer parts, and this “lag” of

the interior temperature will bring about a tendency to instability.

The contraction of the nebula due to cooling will increase the velocity

of rotation, and this again will tend to instability. As a result of

the instability so produced the nebula will change its form, and become

more or less pear-shaped. The narrow end of the pear will then separate

from the body and assume an independent existence as a primitive

planet. This process will recur again and again till the nebula is

resolved into a sun with its attendant planets. The planets, existing

at first as gaseous masses or quasi-gaseous masses, will be liable

to the same kind of transformation, and may thus bud off moons or

satellites.

If the nebula were not in rapid rotation, a slight disturbing cause,

acting at the critical moment when a planet was being ejected, might

determine the inclination of the planet’s orbit, which might thus be

very oblique to the equatorial plane of the nebula. Thus the hypothesis

is not open to one of the objections which have been urged against

that of Laplace--namely, that the orbits of some of the planets in the

solar system are inclined at a large angle with the plane of the sun’s

equator.

[Illustration:

This illustrates Laplace’s theory, which conceived of a vast nebula

filling the whole space of the solar system and rotating around a

central axis. The outer and thinner part had much greater movement

than the denser central mass, finally being thrown off as a ring,

which in turn rolled up into a ball, still following the same

course as the ring had followed. Thus the earth broke off from the

sun and the moon from the earth. The theory is, however, no longer

credited by scientists.

The pear-shaped nebula is the theory of a young English

mathematician, Professor J. H. Jeans. Starting with a spherical

nebula, he argues that in cooling it will assume the form

illustrated above, and that the smaller part will separate and form

a satellite rotating independently but within a distance influenced

by the parent mass.

The spiral nebula in Canes Venatici, a revolving mass of gas or

meteorites, supplies, according to the nebular hypothesis of

Messrs. Chamberlin and Moulton, an excellent example of how the

earth and moon were formed. We may reasonably imagine the smaller

spiral to represent the moon in the act of being thrown off by the

earth.

THREE FAMOUS THEORIES OF THE BEGINNING OF THE EARTH]

[Sidenote: Heavenly Bodies in Collision]

Jeans mentions two disturbing causes in particular which might easily

arise--one the penetration of the nebula by a wandering meteorite,

which might precipitate an event already on the verge of happening,

and simultaneously determine both the birth of a planet and the

obliquity of its orbit; the second, the presence of some distant

mass, such as a star, which, by raising a quasi-tide in the nebula,

would give the final touch required to overturn its equilibrium. The

influence of a distant body, such as a passing star, has been invoked

by Moulton in another version of the nebular hypothesis. In conjunction

with Chamberlin, he calls special attention to the spiral nebulæ, which

are by far the commonest kind, as presenting the closest approach to

the conditions which obtain when planets are actually in course of

formation. Chamberlin and Moulton enter on a detailed account of the

manner in which they suppose the planets to have grown by the gradual

accretion of meteoric masses as these encountered each other while

moving in various elliptical orbits.

At present it would seem impossible to speak with certainty as to

the precise history of the solar system. Meanwhile, we may console

ourselves with the closing words of Professor Jeans’ paper, to the

effect that “no difficulty need be experienced in referring existing

planetary systems to a nebulous or meteoric origin on the ground

that the configurations of these systems are not such as could have

originated out of a rotating mass of liquid.”

An investigation by Sir George Darwin, which has furnished inspiration

to such hypotheses as that of Jeans, brings us nearer the immediate

subject of this essay, since it treats of one of the last acts in the

great drama of planetary existence, and attempts to derive the earth

and moon from a common origin in a single rotating sphere.

[Sidenote: Why the Day is Growing Longer]

It is well known that, owing to the frictional effects produced by the

tides, the earth is being gradually slowed down as it rotates upon

its axis. Thus the day is constantly getting longer, so that in a few

millions of years it will have increased in length from twenty-four

to twenty-five hours. On the other hand, in past time it must have

been shorter than at present: a few millions of years ago it was only

twenty-three hours in length, and many millions of years earlier it

was still less, only some five hours or so. At that time the earth

was hotter than it is now, less rigid, more yielding, and, owing to

its rapid rotation, less stable. The action on the moon of the tides

produced in it by the earth is similar, and the rotation of the moon

has been so far diminished by them that its day has become as long as

the month--_i.e._, our satellite only turns once round on its axis in

the time that it takes to revolve once round the earth; it is for this

reason that our satellite keeps always the same face turned towards us.

[Sidenote: The Moon Was Part of Our Sphere]

The retardation of the earth in its rotation has, however, a very

remarkable effect on the revolution of the moon; it involves--by the

principle of the conservation of moment of momentum--a corresponding

acceleration of the moon in its orbit, and, as a consequence of this,

an enlargement of this orbit--that is, the moon is pushed away from us,

as it were, and thus becomes more remote. But if so, the moon must have

been nearer to us in times past. It is possible to trace the approach

of the moon to the earth as we go backwards in time till the distance

between them was only two and a half terrestrial radii instead of the

sixty radii which now separate them. Mathematics do not take us farther

back than this. But it is difficult to resist the suggestion that in

the immediately preceding stage of development the earth and moon

formed together a single sphere.

If we may adopt this view, then we must regard the sphere as subject to

the tidal influence of the sun. It was much hotter, and therefore more

yielding, than the present earth; it was also rotating much faster,

probably once in about four or five hours. It would be contracting as a

consequence of cooling, and the contraction would lead to instability

(gravitational instability); its rapid rotation would also tend toward

instability (rotational instability). It is difficult to say which

of these two, gravitational or rotational instability, would be the

most effective; but the combined result would be to give a pear-shaped

form to the rotating mass, and eventually to deepen the constriction

between the narrow and the broad end, till the smaller protuberance

became completely dissevered from the larger mass, and so entered on

an independent existence as the moon. This final step in the process

would probably depend on the tide-producing power of the sun; the

larger mass remained behind as the earth, whose individual existence

may be said to date from this event.

[Sidenote: How the Moon Broke Away]

The young earth would be subject to very much the same conditions after

as before the ejection of the moon, and might very possibly again pass

into a pear-shaped form, but without proceeding further through those

subsequent changes, which would have led to the formation of another

satellite; and while possessing some such form as this, she might

very well have consolidated. With advancing years she would lose, as

we have seen, the activity of her youth, the drag of the tides would

cause her to spin ever more slowly on her axis, till the day would

become prolonged to the twenty-four hours of the present. With this

diminished rate of spin, the earth, if free to yield, would lose the

pear-shaped form and become an oblate spheroid, and the oblateness of

this spheroid would continually diminish, so that it would continually

approach towards a true sphere. Suppose, however, that the earth as it

cooled lost its power of readily yielding--and at present it is more

rigid than a globe of steel--then it would pass from form to form,

not by a flowing movement, but by a series of ruptures, and its form

at any moment might be a little in arrear of that which it would have

possessed if it had been in the fluid state.

Thus it might indeed be possible still to discover some trace of an

old-fashioned form in the existing planet; and a careful examination

of the distribution of land and sea as represented on a terrestrial

globe does, in fact, reveal a remarkable symmetry, in which we seem

to recognise a surviving vestige of its early state. The great

continent of Africa projects like the narrow end of a pear; around it

are oceans--the Atlantic, the Indian Ocean, and the Mediterranean Sea,

which was once of far greater extent; then comes a great dismembered

ring of land, the two Americas, the Antarctic continent, Australia,

Asia, and Europe. Within these, on the side opposite to Africa, is the

great Pacific Ocean, which covers over the broad end of the pear.

[Sidenote: Earth’s Unknown Changes]

[Illustration: THE SHAPING OF THE FACE OF THE EARTH

Soon after the earth had cooled down, so that the oceans were

formed, the shaping of the great continents began. The action of

moving water in the making of new land is well illustrated by the

vast delta of the Mississippi, where an area larger than Wales has

been formed by debris deposited by the river.

]

A line drawn from somewhere in Central Africa to its antipodes in the

Pacific, through the centre of the earth, would correspond to the long

axis of the pear; a second, at right angles to this, would correspond

to its breadth; and a third, at right angles to both, would correspond

to the axis on which it rotates. A diameter of the earth taken through

the equator is almost 8,000 miles in length, the Polar diameter is

about sixteen miles shorter, and this slight difference measures the

oblateness of the spheroid, or the departure of the form of the earth

from a true sphere. Further, it would appear that the diameter drawn

through Africa is about half a mile longer than the equatorial diameter

taken at right angles to it, and this insignificant quantity measures

the departure of the form of the earth from that of an oblate spheroid

to that of a pear, so nearly complete is the adjustment of its form to

existing conditions. Before this nice adjustment was reached, the earth

must have suffered many changes, passed through many times of stress

and storm, and witnessed many geological revolutions.

[Sidenote: An Age of Red-hot Rain!]

If, at the beginning of her career, the earth was molten, or at a

very high temperature, she must have been surrounded by a very deep

and dense atmosphere, for all the waters which now rest on her

surface--oceans, lakes, and rivers--would have contributed to it in the

state of steam; and not till the temperature of the ground had fallen

to 380 deg. C. could liquid water have begun to accumulate. Then a

steady downpour of almost red-hot rain would have set in, filling up

the neck of the pear and extending far and wide over its broad end.

The temperature would now fall somewhat rapidly, and in a short space

of time the surface of the earth would have become as cool as it is at

the present day. Directly the waters of the firmament had collected

into the oceans, leaving behind an atmosphere like that which now

exists, geological agencies of the kind we are now familiar with would

begin their sway. Air and rain would exert their insidious power upon

the rocks, sapping their strength, converting the hardest granite into

soft sand and clay, which would be washed away by the rain through

brooks and rivulets into the channels of many rivers, all hastening

with their burden of sediment, to deposit it finally in the sea. Here

it would accumulate, layer after layer, building up those mighty masses

of strata which now form the greater part of the visible land. While

this general action was everywhere in progress, wearing down continents

and islands towards the level of the sea, more specialised activities

were assisting to the same end.

[Illustration: TWO STAGES IN THE LIFE OF THE EARTH

This illustrates in striking manner, based on the calculations

of the best authorities, the comparative sizes of the earth,

first as a gaseous mass, and, second, after it had cooled down

and solidified into the planet on which we live. The small dot

represents 8,000 miles, the earth’s diameter.

]

The waves which fall upon our coasts are now constantly undermining

the cliffs and extending the margin of the sea at the expense of the

land, and rivers not only serve to transport sediment, but cut down

their channels deep into the rock, and so carve out the most varied

landscapes of hill and valley from monotonous tableland.

[Sidenote: Action of Winds and Tides]

When we enter into calculations we are astonished at the rapidity

with which these agents perform their work even at the present day;

but as we proceed farther back into the past, when the earth was full

of youthful energy, their power must have been greatly enhanced. We

might almost take the measure of the day as the measure of their

work, for they probably accomplished as much during the eight hours’

day which once existed as they do now in twenty-four hours. A little

consideration will make this clear. It is the winds which, blowing

over the surface of the ocean, produce the sea waves, and it is these

falling on our coasts that perform the work of marine denudation. But

the winds are due in the first place to the heat of the sun, and the

difference of temperature established at the equator and the poles;

and, in the next place, to the rotation of the earth. Thus, with the

increased rapidity of rotation which we know to have existed, and

with increased radiation from the sun, a very probable contingency,

the winds would increase in strength and more powerfully erode our

coasts. Again, with the moon in greater proximity, and with a more

rapid rotation of the earth, the tides would be much higher and more

frequent, and these, raising and lowering the cutting edge of the sea,

greatly assist it in its work of destruction. The winds and the tides

produce various marine currents, and these help to distribute the

sediment which the rivers deliver into the sea, so that when stronger

currents flowed as a result of more powerful tides and more violent

winds, the sediments would be strewn over wider areas; hence, the more

ancient strata of our planet are far more widely distributed than are

those of later time.

[Illustration: THREE VIEWS OF THE GLOBE SHOWING HOW THE GREAT MOUNTAIN

RANGES WERE FORMED

In the days when the earth’s crust had formed but was still

unstable, the process of cooling not having gone far enough,

there would not be the mountains which now characterise it. These

came when the earth contracted and crumpled up along certain

well defined lines, which are now represented by the three great

mountain chains of the world.

]

[Sidenote: Building Up the Earth]

Finally, a heavier rainfall would result from a more active atmospheric

circulation, creating larger rivers, and thus, at the beginning, all

those denuding agents which are engaged in wearing the land down into

the sea would be working at a more rapid pace. Correspondingly, all

the agents which are occupied in building up deposits of sediments

would have extended their operations over a wider area, laying down a

foundation broad and deep.

On the other hand, the contraction of the earth, due to the loss of

its energy of rotation as well as of its internal heat, would also

have proceeded more rapidly, new land would have emerged from the sea,

old lands would have been submerged beneath it far less slowly than at

the present day; ruptures of the crust, accompanied by earthquakes and

volcanic action, would have been more frequent and thus, by the more

rapid loss of its intrinsic energy, the renovation of the earth would

have kept pace with its accelerated destruction.

One effect of the contraction of the earth which has manifested itself

in even late geological times is the crumpling up of the terrestrial

crust into the sharp folds of mountain chains; but at the beginning

this crumpling must have been far more universal and energetic. In this

connection it is interesting to observe that the most ancient rocks

known to us--the Archæan--never present themselves under any other form

than as intensely plicated masses. They originally consisted of lava

flows and volcanic ashes, of ancient sediments and limestones, into

which subterranean masses of granite and other molten, deep-seated

rocks have been injected; but under the intense pressures to which

they were subjected after their formation they and the invading

granite have entirely lost their original character, and have been

metamorphosed into gneisses, schists, and marble, all sharply and

closely folded together. In any given district the direction of their

folding is maintained with wonderful constancy over great distances.

There is no succeeding system of rocks that has been so completely

transformed, so universally plicated, as this ancient Archæan complex.

In later times we can pass from stratum to stratum of the sedimentary

series and read their history almost as we turn over the pages of a

book; in the Archæan all are kneaded together into a state of such

desperate entanglement as to defy the powers of human ingenuity to

unravel them. Thus the line of demarcation between the Archæan and

subsequent sedimentary systems is the sharpest and most absolute that

is known to us in the history of the earth. It marks the close of our

planet’s infancy, the several events of which have passed into oblivion

as profound as that of our own forgetfulness of our earliest days.

Later events, on the other hand, are recorded in the stratified series

with a faithfulness which increases as we approach existing times.

[Sidenote: How We Know These Wonders]

[Sidenote: The Ocean 100 million Years old!]

[Sidenote: The Part Radium may play]

The Book of History (Vol. 1 of 18) A History of All Nations from the Earliest Times to the Present · 第 12 / 58 段