CHAPTER IX

_THEORIES OF PLANETARY EVOLUTION_

We cannot doubt that the solar system, as we see it, is the result of

some process of growth--that, during innumerable ages, the forces of

Nature were at work upon its materials, blindly modelling them into the

shape appointed for them from the beginning by Omnipotent Wisdom. To set

ourselves to inquire what that process was may be an audacity, but it is

a legitimate, nay, an inevitable one. For man's implanted instinct to

"look before and after" does not apply to his own little life alone, but

regards the whole history of creation, from the highest to the

lowest--from the microscopic germ of an alga or a fungus to the visible

frame and furniture of the heavens.

Kant considered that the inquiry into the mode of origin of the world

was one of the easiest problems set by Nature; but it cannot be said

that his own solution of it was satisfactory. He, however, struck out in

1755 a track which thought still pursues. In his _Allgemeine

Naturgeschichte_ the growth of sun and planets was traced from the

cradle of a vast and formless mass of evenly diffused particles, and the

uniformity of their movements was sought to be accounted for by the

unvarying action of attractive and repulsive forces, under the dominion

of which their development was carried forward.

In its modern form, the "Nebular Hypothesis" made its appearance in

1796.[1150] It was presented by Laplace with diffidence, as a

speculation unfortified by numerical buttresses of any kind, yet with

visible exultation at having, as he thought, penetrated the birth-secret

of our system. He demanded, indeed, more in the way of postulates than

Kant had done. He started with a sun ready made,[1151] and surrounded

with a vast glowing atmosphere, extending into space out beyond the

orbit of the farthest planet, and endowed with a slow rotatory motion.

As this atmosphere or nebula cooled, it contracted; and as it

contracted, its rotation, by a well-known mechanical law, became

accelerated. At last a point arrived when tangential velocity at the

equator increased beyond the power of gravity to control, and

equilibrium was restored by the separation of a nebulous ring revolving

in the same period as the generating mass. After a time, the ring broke

up into fragments, all eventually reunited in a single revolving and

rotating body. This was the first and farthest planet.

Meanwhile the parent nebula continued to shrink and whirl quicker and

quicker, passing, as it did so, through successive crises of

instability, each resulting in, and terminated by, the formation of a

planet, at a smaller distance from the centre, and with a shorter period

of revolution than its predecessor. In these secondary bodies the same

process was repeated on a reduced scale, the birth of satellites ensuing

upon their contraction, or not, according to circumstances. Saturn's

ring, it was added, afforded a striking confirmation of the theory of

annular separation,[1152] and appeared to have survived in its original

form in order to throw light on the genesis of the whole solar system;

while the four first discovered asteroids offered an example in which

the _débris_ of a shattered ring had failed to coalesce into a single

globe.

This scene of cosmical evolution was a characteristic bequest from the

eighteenth century to the nineteenth. It possessed the self-sufficing

symmetry and entireness appropriate to the ideas of a time of

renovation, when the complexity of nature was little accounted of in

comparison with the imperious orderliness of the thoughts of man. Since

its promulgation, however, knowledge has transgressed many boundaries,

and set at naught much ingenious theorising. How has it fared with

Laplace's sketch of the origin of the world? It has at least not been

discarded as effete. The groundwork of speculation on the subject is

still furnished by it. It is, nevertheless, admittedly inadequate. Of

much that exists it gives no account, or an erroneous one. The march of

events certainly did not everywhere--even if it did anywhere--follow the

exact path prescribed for it. Yet modern science attempts to supplement,

but scarcely ventures to supersede it.

Thought has, in many directions, been profoundly modified by Mayer's and

Joule's discovery, in 1842, of the equivalence between heat and motion.

Its corollary was the grand idea of the "conservation of energy," now

one of the cardinal principles of science. This means that, under the

ordinary circumstances of observation, the old maxim _ex nihilo nihil

fit_ applies to force as well as to matter. The supplies of heat, light,

electricity, must be kept up, or the stream will cease to flow. The

question of the maintenance of the sun's heat was thus inevitably

raised; and with the question of maintenance that of origin is

indissolubly connected.

Dr. Julius Robert Mayer, a physician residing at Heilbronn, was the

first to apply the new light to the investigation of what Sir John

Herschel had termed the "great secret." He showed that if the sun were a

body either simply cooling or in a state of combustion, it must long

since have "gone out." Had an equal mass of coal been set alight four or

five centuries after the building of the Pyramid of Cheops, and kept

burning at such a rate as to supply solar light and heat during the

interim, only a few cinders would now remain in lieu of our undiminished

glorious orb. Mayer looked round for an alternative. He found it in the

"meteoric hypothesis" of solar conservation.[1153] The importance in the

economy of our system of the bodies known as falling stars was then (in

1848) beginning to be recognised. It was known that they revolved in

countless swarms round the sun; that the earth daily encountered

millions of them; and it was surmised that the cone of the zodiacal

light represented their visible condensation towards the attractive

centre. From the zodiacal light, then, Mayer derived the store needed

for supporting the sun's radiations. He proved that, by the stoppage of

their motion through falling into the sun, bodies would evolve from

4,600 to 9,200 times as much heat (according to their ultimate velocity)

as would result from the burning of equal masses of coal, their

precipitation upon the sun's surface being brought about by the

resisting medium observed to affect the revolutions of Encke's comet.

There was, however, a difficulty. The quantity of matter needed to keep,

by the sacrifice of its movement, the hearth of our system warm and

bright would be very considerable. Mayer's lowest estimate put it at

94,000 billion kilogrammes per second, or a mass equal to that of our

moon bi-annually. But so large an addition to the gravitating power of

the sun would quickly become sensible in the movement of the bodies

dependent upon him. Their revolutions would be notably accelerated.

Mayer admitted that each year would be shorter than the previous one by

a not insignificant fraction of a second, and postulated an unceasing

waste of substance, such as Newton had supposed must accompany emission

of the material corpuscles of light, to neutralise continual

reinforcement.

Mayer's views obtained a very small share of publicity, and owned Mr.

Waterston as their independent author in this country. The meteoric, or

"dynamical," theory of solar sustentation was expounded by him before

the British Association in 1853. It was developed with his usual ability

by Lord Kelvin, in the following year. The inflow of meteorites, he

remarked, "is the only one of all conceivable causes of solar heat which

we know to exist from independent evidence."[1154] We know it to exist,

but we now also know it to be entirely insufficient. The supplies

presumed to be contained in the zodiacal light would be quickly

exhausted; a constant inflow from space would be needed to meet the

demand. But if moving bodies were drawn into the sun at anything like

the required rate, the air, even out here at ninety-three millions of

miles distance, would be thick with them; the earth would be red-hot

from their impacts;[1155] geological deposits would be largely

meteoric;[1156] to say nothing of the effects on the mechanism of the

heavens. Lord Kelvin himself urged the inadmissibility of the

"extra-planetary" theory of meteoric supply on the very tangible ground

that, if it were true, the year would be shorter now, actually by six

weeks, than at the opening of the Christian era. The "intra-planetary"

supply, however, is too scanty to be anything more than a temporary

makeshift.

The meteoric hypothesis was naturally extended from the maintenance of

the sun's heat to the formation of the bodies circling round him. The

earth--no less doubtless than the other planets--is still growing.

Cosmical matter in the shape of falling stars and aërolites, to the

amount, adopting Professor Newton's estimate, of 100 tons daily, is

swept up by it as it pursues its orbital round. Inevitably the idea

suggested itself that this process of appropriation gives the key to the

life-history of our globe, and that the momentary streak of fire in the

summer sky represents a feeble survival of the glowing hailstorm by

which in old times it was fashioned and warmed. Mr. E. W. Brayley

supported this view of planetary production in 1864,[1157] and it has

recommended itself to Haidinger, Helmholtz, Proctor, and Faye. But the

negative evidence of geological deposits appears fatal to it.

The theory of solar energy now generally regarded as the true one was

enounced by Helmholtz in a popular lecture in 1854. It depends upon the

same principle of the equivalence of heat and motion which had suggested

the meteoric hypothesis. But here the movement surrendered and

transformed belongs to the particles, not of any foreign bodies, but of

the sun itself. Drawn together from a wide ambit by the force of their

own gravity, their fall towards the sun's centre must have engendered a

vast thermal store, of which 453/454 are computed to be already spent.

Presumably, however, this stream of reinforcement is still flowing. In

the very act of parting with heat, the sun develops a fresh stock. His

radiations, in short, are the direct result of shrinkage through

cooling. A diminution of the solar diameter by 380 feet yearly would

just suffice to cover the present rate of emission, and would for ages

remain imperceptible with our means of observation, since, after the

lapse of 6,000 years, the lessening of angular size would scarcely

amount to one second.[1158] But the process, though not terminated, is

strictly a terminable one. In less than five million years, the sun will

have contracted to half its present bulk. In seven million more, it will

be as dense as the earth. It is difficult to believe that it will then

be a luminous body.[1159] Nor can an unlimited past duration be

admitted. Helmholtz considered that radiation might have gone on with

its actual intensity for twenty-two, Langley allows only eighteen

million years. The period can scarcely be stretched, by the most

generous allowances, to double the latter figure. But this is far from

meeting the demands of geologists and biologists.

An attempt was made in 1881 to supply the sun with machinery analogous

to that of a regenerative furnace, enabling it to consume the same fuel

over and over again, and so to prolong indefinitely its beneficent

existence. The inordinate "waste" of energy, which shocks our thrifty

ideas, was simultaneously abolished. The earth stops and turns variously

to account one 2,250-millionth part of the solar radiations; each of the

other planets and satellites takes a proportionate share; the rest,

being all but an infinitesmal fraction of the whole, is dissipated

through endless space, to serve what purpose we know not. Now, on the

late Sir William Siemens's plan, this reckless expenditure would cease;

the solar incomings and outgoings would be regulated on approved

economic principles, and the inevitable final bankruptcy would be staved

off to remote ages.

But there was a fatal flaw in its construction. He imagined a perpetual

circulation of combustible materials, alternately surrendering and

regaining chemical energy, the round being kept going by the motive

force of the sun's rotation.[1160] This, however, was merely to perch

the globe upon a tortoise, while leaving the tortoise in the air. The

sun's rotation contains a certain definite amount of mechanical

power--enough, according to Lord Kelvin, if directly converted into

heat, to keep up the sun's emission during 116 years and six days--a

mere moment in cosmical time. More economically applied, it would no

doubt go farther. Its exhaustion would, nevertheless, under the most

favourable circumstances, ensue in a comparatively short period.[1161]

Many other objections equally unanswerable have been urged to the

"regenerative" hypothesis, but this one suffices.

Dr. Croll's collision hypothesis[1162] is less demonstrably unsound, but

scarcely less unsatisfactory. By the mutual impact of two dark masses

rushing together with tremendous speed, he sought to provide the solar

nebula with an immense _original_ stock of heat for the reinforcement of

that subsequently evolved in the course of its progressive contraction.

The sun, while still living on its capital, would thus have a larger

capital to live on, and the time-demands of the less exacting geologists

and biologists might be successfully met. But the primitive event,

assumed for the purpose of dispensing them from the inconvenience of

"hurrying up their phenomena," is not one that a sane judgment can

readily admit to have ever, in point of actual fact, happened.

There remains, then, as the only intelligible rationale of solar

sustentation, Helmholtz's shrinkage theory. And this has a very

important bearing upon the nebular view of planetary formation; it may,

in fact, be termed its complement. For it involves the idea that the

sun's materials, once enormously diffused, gradually condensed to their

present volume with development of heat and light, and, it may plausibly

be added, with the separation of dependent globes. The data furnished by

spectrum analysis, too, favour the supposition of a common origin for

sun and planets by showing their community of substance; while gaseous

nebulæ present examples of vast masses of tenuous vapour, such as our

system may plausibly be conjectured to have primitively sprung from.

But recent science raises many objections to the details, if it supplies

some degree of confirmation to the fundamental idea of Laplace's

cosmogony. The detection of the retrograde movement of Neptune's

satellite made it plain that the anomalous conditions of the Uranian

world were due to no extraordinary disturbance, but to a systematic

variety of arrangement at the outskirts of the solar domain. So that,

were a trans-Neptunian planet discovered, we should be fully prepared to

find it rotating, and surrounded by satellites circulating from east to

west. The uniformity of movement, upon the probabilities connected with

which the French geometer mainly based his scheme, thus at once

vanishes.

The excessively rapid revolution of the inner Martian moon is a further

stumbling-block. On Laplace's view, _no_ satellite can revolve in a

shorter time than its primary rotates; for in its period of circulation

survives the period of rotation of the parent mass which filled the

sphere of its orbit at the time of giving it birth. And rotation

quickens as contraction goes on; therefore, the older time of axial

rotation should invariably be the longer. This obstacle can, however, as

we shall presently see, be turned.

More serious is one connected with the planetary periods, pointed out by

Babinet in 1861.[1163] In order to make them fit in with the hypothesis

of successive separation from a rotating and contracting body, certain

arbitrary assumptions have to be made of fluctuations in the

distribution of the matter forming that body at the various epochs of

separation.[1164] Such expedients usually merit the distrust which they

inspire. Primitive and permanent irregularities of density in the solar

nebula, such as Miss Young's calculations suggest,[1165] do not, on the

other hand, appear intrinsically improbable.

Again, it was objected by Professor Kirkwood in 1869[1166] that there

could be no sufficient cohesion in such an enormously diffused mass as

the planets are supposed to have sprung from to account for the wide

intervals between them. The matter separated through the growing excess

of centrifugal speed would have been cast off, not by rarely recurring

efforts, but continually, fragmentarily, _pari passu_ with condensation

and acceleration. Each wisp of nebula, as it found itself unduly

hurried, would have declared its independence, and set about revolving

and condensing on its own account. The result would have been a

meteoric, not a planetary system.

Moreover, it is a question whether the relative ages of the planets do

not follow an order just the reverse of that concluded by Laplace.

Professor Newcomb holds the opinion that the rings which eventually

constituted the planets divided from the main body of the nebula almost

simultaneously, priority, if there were any, being on the side of the

inner and smaller ones;[1167] while in M. Faye's cosmogony,[1168] the

retrograde motion of the systems formed by the two outer planets is

ascribed--on grounds, it is true, of dubious validity--to their

comparatively late origin.

This ingenious scheme was designed, not merely to complete, but to

supersede that of Laplace, which, undoubtedly, through the inclusion by

our system of oppositely directed rotations, forfeits its claim simply

and singly to account for the fundamental peculiarities of its

structure.

M. Faye's leading contention is that, under the circumstances assumed by

Laplace, not the two outer planets alone, but the whole company must

have been possessed of retrograde rotation. For they were formed--_ex

hypothesi_--after the sun; central condensation had reached an advanced

stage when the rings they were derived from separated; the principle of

inverse squares consequently held good, and Kepler's Laws were in full

operation. Now, particles circulating in obedience to these laws can

only--since their velocity decreases outward from the centre of

attraction--coalesce into a globe with a _backward_ axial movement. Nor

was Laplace blind to this flaw in his theory; but his effort to remove

it, though it passed muster for the best part of a century,[1169] was

scarcely successful. His planet-forming rings were made to rotate _all

in one piece_, their outer parts thus necessarily travelling at a

swifter linear rate than their inner parts, and eventually uniting,

equally of necessity, into a _forward_-spinning body. The strength of

cohesion involved may, however, safely be called impossible, especially

when it is considered that nebulous materials were in question.

The reform proposed by M. Faye consists in admitting that all the

planets inside Uranus are of pre-solar origin--that they took globular

form in the bosom of a nearly homogeneous nebula, revolving in a single

period, with motion accelerated from centre to circumference, and hence

agglomerating into masses with a direct rotation. Uranus and Neptune owe

their exceptional characteristics to their later birth. When they came

into existence, the development of the sun was already far advanced,

central force had acquired virtually its present strength, unity of

period had been abolished by its predominance, and motion was retarded

outward.

Thus, what we may call the relative chronology of the solar system is

thrown once more into confusion. The order of seniority of the planets

is now no easier to determine than the "Who first, who last?" among the

victims of Hector's spear. For M. Faye's arrangements, notwithstanding

the skill with which he has presented them, cannot be unreservedly

accepted. The objections to them, thoughtfully urged by M. C. Wolf[1170]

and Professor Darwin,[1171] are grave. Not the least so is his omission

to take account of an agency of change presently to be noticed.

A further valuable discussion of the matter was published by M. du

Ligondès in 1897.[1172] His views are those of Faye, modified to disarm

the criticisms they had encountered; and special attention may be

claimed for his weighty remark that each planet has a life-history of

its own, essentially distinct from those of the others, and, despite

original unity, not to be confounded with them. The drift of recent

investigations seems, indeed, to be to find the embryonic solar system

already potentially complete in the parent nebula, like the oak in an

acorn, and to relegate detailed explanations of its peculiarities to the

dim pre-nebular fore-time.

We now come to a most remarkable investigation--one, indeed, unique in

its profession to lead us back with mathematical certainty towards the

origin of a heavenly body. We refer to Professor Darwin's inquiries into

the former relations of the earth and moon.[1173]

They deal exclusively with the effects of tidal friction, and primarily

with those resulting, not from oceanic, but from "bodily" tides, such as

the sun and moon must have raised in past ages on a liquid or viscous

earth. The immediate effect of either is, as already explained, to

destroy the rotation of the body on which the tide is raised, as regards

the tide-raising body, bringing it to turn always the same face towards

its disturber. This, we can see, has been completely brought about in

the case of the moon. There is, however, a secondary or reactive effect.

Action is always mutual. Precisely as much as the moon pulls the

terrestrial tidal wave backward, the tidal wave pulls the moon forward.

But pulling a body forward in its orbit implies the enlargement of that

orbit; in other words, the moon is, as a consequence of tidal friction,

very slowly receding from the earth. This will go on (other

circumstances remaining unchanged) until the lengthening day overtakes

the more tardily lengthening month, when each will be of about 1,400

hours.[1174] A position of what we may call tidal equilibrium between

earth and moon will (apart from disturbance by other bodies) then be

attained.

If, however, it be true that, in the time to come, the moon will be much

farther from us, it follows that in the time past she was much nearer to

us than she now is. Tracing back her history by the aid of Professor

Darwin's clue, we at length find her revolving in a period of somewhere

between two and four hours, almost in contact with an earth rotating

just at the same rate. This was before tidal friction had begun its work

of grinding down axial velocity and expanding orbital range. But the

position was not one of stable equilibrium. The slightest inequality

must have set on foot a series of uncompensated changes. If the moon had

whirled the least iota faster than the earth spun she must have been

precipitated upon it. Her actual existence shows that the trembling

balance inclined the other way. By a second or two to begin with, the

month exceeded the day; the tidal wave crept ahead of the moon; tidal

friction came into play, and our satellite started on its long spiral

journey outward from the parent globe. This must have occurred, it is

computed, _at least_ fifty-four million years ago.

That this kind of tidal reactive effect played its part in bringing the

moon into its present position, and is still, to some slight extent, at

work in changing it, there can be no doubt whatever. An irresistible

conjecture carried the explorer of its rigidly deducible consequences

one step beyond them. The moon's time of revolution, when so near the

earth as barely to escape contact with it, must have been, by Kepler's

Law, more than two and less than two and a half hours. Now it happens

that the most rapid rate of rotation of a fluid mass of the earth's

average density, consistent with spheroidal equilibrium, is two hours

and twenty minutes. Quicken the movement but by one second and the globe

must fly asunder. Hence the inference that the earth actually _did_ fly

asunder through over-fast spinning, the ensuing disruption representing

the birth-throes of the moon. It is likely that the event was hastened

or helped by solar tidal disturbance.

To recapitulate. Analysis tracks backward the two bodies until it leaves

them in very close contiguity, one rotating and the other revolving in

approximately the same time, and that time certainly not far different

from, and quite possibly identical with, the critical period of

instability for the terrestrial spheroid. "Is this," Professor Darwin

asks, "a mere coincidence, or does it not rather point to the break-up

of the primeval planet into two masses in consequence of a too rapid

rotation?"[1175]

We are tempted, but are not allowed to give an unqualified assent. Mr.

James Nolan of Victoria has made it clear that the moon could not have

subsisted as a continuous mass under the powerful disruptive strain

which would have acted upon it when revolving almost in contact with the

present surface of the earth; and Professor Darwin, admitting the

objection, concedes to our satellite, in its initial stage, the

alternative form of a flock of meteorites.[1176] But such a congregation

must have been quickly dispersed, by tidal action, into a meteoric ring.

The same investigator subsequently fixed 6,500 miles from centre to

centre as the minimum distance at which the moon could have revolved in

its entirety; and he concluded it "necessary to suppose that, after the

birth of a satellite, if it takes place at all in this way, a series of

changes occur which are quite unknown."[1177] The evidence, however, for

the efficiency of tidal friction in bringing about the actual

configuration of the lunar-terrestrial system is not invalidated by this

failure to penetrate its natal mystery. Under its influence the

principal elements of that system fall into interdependent mutual

relations. It connects, casually and quantitatively, the periods of the

moon's revolution and of the earth's rotation, the obliquity of the

ecliptic, the inclination and eccentricity of the lunar orbit. All this

can scarcely be accidental.

Professor Darwin's first researches on this subject were communicated to

the Royal Society, December 18, 1879. They were followed, January 20,

1881,[1178] by an inquiry on the same principles into the earlier

condition of the entire solar system. The results were a warning against

hasty generalisation. They showed that the lunar-terrestrial system, far

from being a pattern for their development, was a singular exception

among the bodies swayed by the sun. Its peculiarity resides in the fact

that the moon is _proportionately_ by far the most massive attendant

upon any known planet. Its disturbing power over its primary is thus

abnormally great, and tidal friction has, in consequence, played a

predominant part in bringing their mutual relations into their present

state.

The comparatively late birth of the moon tends to ratify this inference.

The dimensions of the earth did not differ (according to our present

authority) very greatly from what they now are when her solitary

offspring came, somehow, into existence. This is found not to have been

the case with any other of the planets. It is unlikely that the

satellites of Jupiter, Saturn, or Mars (we may safely add, of Uranus or

Neptune) ever revolved in much narrower orbits than those they now

traverse; it is practically certain that they did not, like our moon,

originate very near the _present_ surfaces of their primaries.[1179]

What follows? The tide-raising power of a body grows with vicinity in a

rapidly accelerated ratio. Lunar tides must then have been on an

enormous scale when the moon swung round at a fraction of its actual

distance from the earth. But no other satellite with which we are

acquainted occupied at any time a corresponding position. Hence no other

satellite ever possessed tide-raising capabilities in the least

comparable to those of the moon. We conclude once more that tidal

friction had an influence here very different from its influence

elsewhere. Quite possibly, however, that influence may be more nearly

spent than in less advanced combinations of revolving globes. Mr. Nolan

concluded in 1895[1180] that it still retains appreciable efficacy in

the several domains of the outer planets. The moons of Jupiter and

Saturn are, by his calculations, in course of sensible retreat, under

compulsion of the perennial ripples raised by them on the surfaces of

their gigantic primaries. He thus connects the interior position of the

fifth Jovian satellite with its small mass. The feebleness of its

tide-raising power obliged it to remain behind its companions; for there

is no sign of its being more juvenile than the Galilean quartette.

The yielding of plastic bodies to the strain of unequal attractions is a

phenomenon of far-reaching consequence. We know that the sun as well as

the moon causes tides in our oceans. There must, then, be solar, no less

than lunar, tidal friction. The question at once arises: What part has

it played in the development of the solar system? Has it ever been one

of leading importance, or has its influence always been, as it now is,

subordinate, almost negligible? To this, too, Professor Darwin supplies

an answer.

It can be stated without hesitation that the sun did _not_ give birth to

the planets, as the earth has been supposed to have given birth to the

moon, by the disruption of its already condensed, though viscous and

glowing mass, pushing them then gradually backward from its surface into

their present places. For the utmost possible increase in the length of

the year through tidal friction is one hour; and five minutes is a more

probable estimate.[1181] So far as the pull of tide-waves raised on the

sun by the planets is concerned, then, the distances of the latter have

never been notably different from what they now are; though that cause

may have converted the paths traversed by them from circles into

ellipses.

Over their _physical_ history, however, it was probably in a large

measure influential. The first vital issue for each of them

was--satellites or no satellites? Were they to be governors as well as

governed, or should they revolve in sterile isolation throughout the

æons of their future existence? Here there is strong reason to believe

that solar tidal friction was the overruling power. It is remarkable

that planetary fecundity increases--at least so far outward as

Saturn--with distance from the sun. Can these two facts be in any way

related? In other words, is there any conceivable way by which tidal

influence could prevent or impede the throwingoff of secondary bodies?

We have only to think for a moment in order to see that this is

precisely one of its direct results.[1182]

Tidal friction, whether solar or lunar, tends to reduce the axial

movement of the body it acts upon. But the separation of satellites

depends--according to the received view--upon the attainment of a

disruptive rate of rotation. Hence, if solar tidal friction were strong

enough to keep down the pace below this critical point, the contracting

mass would remain intact--there would be no satellite-production. This,

in all probability, actually occurred in the case both of Mercury and

Venus. They cooled without dividing, because the solar friction-brake

applied to them was too strong to permit acceleration to pass the limit

of equilibrium. The complete destruction of their relative axial

movement has been rendered probable by recent observations; and that the

process went on rapidly is a reasonable further inference. The earth

barely escaped the fate of loneliness incurred by her neighbours. Her

first and only epoch of instability was retarded until she had nearly

reached maturity. The late appearance of the moon accounts for its large

relative size--through the increased cohesion of an already strongly

condensed parent mass--and for the distinctive peculiarities of its

history and influence on the producing globe.

Solar tidal friction, although it did not hinder the formation of two

minute dependents of Mars, has been invoked to explain the anomalously

rapid revolution of one of them. Phobos, we have seen, completes more

than three revolutions while Mars rotates once. But this was probably

not always so. The two periods were originally nearly equal. The

difference, it is alleged, was brought about by tidal waves raised by

the sun on the semi-fluid spheroid of Mars. Rotatory velocity was

thereby destroyed, the Martian day slowly lengthened, and, as a

secondary consequence, the period of the inner satellite, become shorter

than the augmented day, began progressively to diminish. So that Phobos,

unlike our moon, was in the beginning farther from its primary than now.

But here again Mr. Nolan entered a _caveat_. Applying the simple test of

numerical evaluation, he showed that before solar tidal friction could

lengthen the rotation-period of Mars by so much as one minute, Phobos

should have been precipitated upon its surface.[1183] For the enormous

disparity of mass between it and the sun is so far neutralised by the

enormous disparity in their respective distances from Mars that solar

tidal force there is only fifty times that of the little satellite. But

the tidal effects of a satellite circulating quicker than its primary

rotates exactly reverse those of one moving, like our moon,

comparatively slowly, so that the tides raised by Phobos tend to

_shorten_ both periods. Its orbital momentum, however, is so extremely

small in proportion to the rotational momentum of Mars, that any

perceptible inroad upon the latter is attended by a lavish and ruinous

expenditure of the former. It is as if a man owning a single five-pound

note were to play for equal stakes with a man possessing a million. The

bankruptcy sure to ensue is typified by the coming fate of the Martian

inner satellite. The catastrophe of its fall needs to bring it about

only a very feeble reactive pull compared with the friction which the

sun should apply in order to protract the Martian day by one minute. And

from the proportionate strength of the forces at work, it is quite

certain that one result cannot take place without the other. Nor can

things have been materially different in the past; hence the idea must

be abandoned that the primitive time of rotation of Mars survives in the

period of its inner satellite.

The anomalous shortness of the latter may, however, in M. Wolf's

opinion,[1184] be explained by the "traînées elliptiques" with which

Roche supplemented nebular annulation.[1185] These are traced back to

the descent of separating strata from the _shoulders_ of the great

nebulous spheroid towards its equatorial plane. Their rotational

velocity being thus relatively small, they formed "inner rings," very

much nearer to the centre of condensation than would have been possible

on the unmodified theory of Laplace. Phobos might, in this view, be

called a polar offset of Mars; and the rings of Saturn are thought to

own a similar origin.

Outside the orbit of Mars, solar tidal friction can scarcely be said to

possess at present any sensible power. But it is far from certain that

this was always so. It seems not unlikely that its influence was the

overruling one in determining the direction of planetary rotation. M.

Faye, as we have seen, objected to Laplace's scheme that only retrograde

secondary systems could be produced by it. In this he was anticipated by

Kirkwood, who, however, supplied an answer to his own objection.[1186]

Sun-raised tides must have acted with great power on the diffused masses

of the embryo planets. By their means they doubtless very soon came to

turn (in lunar fashion) the same hemisphere always towards their centre

of motion. This amounts to saying that even if they started with

retrograde rotation, it was, by solar tidal friction, quickly rendered

direct.[1187] For it is scarcely necessary to point out that a planet

turning an invariable face to the sun rotates in the same direction in

which it revolves, and in the same period. As, with the progress of

condensation, tides became feebler and rotation more rapid, the

accelerated spinning necessarily proceeded in the sense thus prescribed

for it. Hence the backward axial movements of Uranus and Neptune may

very well be a survival, due to the inefficiency of solar tides at their

great distance, of a state of things originally prevailing universally

throughout the system.

The general outcome of Mr. Darwin's researches has been to leave

Laplace's cosmogony untouched. He concludes nothing against it, and,

what perhaps tells with more weight in the long run, has nothing to

substitute for it. In one form or the other, if we speculate at all on

the development of the planetary system, our speculations are driven

into conformity with the broad lines of the Nebular Hypothesis--to the

extent, at least, of admitting an original material unity and motive

uniformity. But we can see now, better than formerly, that these supply

a bare and imperfect sketch of the truth. We should err gravely were we

to suppose it possible to reconstruct, with the help of any knowledge

our race is ever likely to possess, the real and complete history of our

admirable system. "The subtlety of nature," Bacon says, "transcends in

many ways the subtlety of the intellect and senses of man." By no mere

barren formula of evolution, indiscriminately applied all round, the

results we marvel at, and by a fragment of which our life is

conditioned, were brought forth; but by the manifold play of interacting

forces, variously modified and variously prevailing, according to the

local requirements of the design they were appointed to execute.

FOOTNOTES:

[Footnote 1150: _Exposition du Système du Monde_, t. ii., p. 295.]

[Footnote 1151: In later editions a retrospective clause was added

admitting a prior condition of all but evanescent nebulosity.]

[Footnote 1152: _Méc. Cél._, lib. xiv., ch. iii.]

[Footnote 1153: _Beiträge zur Dynamik des Himmels_, p. 12.]

[Footnote 1154: _Trans. Roy. Soc. of Edinburgh_, vol. xxi., p. 66.]

[Footnote 1155: Newcomb, _Pop. Astr._, p. 521 (2nd ed.).]

[Footnote 1156: M. Williams, _Nature_, vol. iii., p. 26.]

[Footnote 1157: _Comp. Brit. Almanac_, p. 94.]

[Footnote 1158: Radau, _Bull. Astr._, t. ii., p. 316.]

[Footnote 1159: Newcomb, _Pop. Astr._, pp. 521-525.]

[Footnote 1160: _Proc. Roy. Soc._, vol. xxxiii., p. 393.]

[Footnote 1161: To this hostile argument, as urged by Mr. E. Douglas

Archibald, Sir W. Siemens opposed the increase of rotative velocity

through contraction (_Nature_, vol. xxv., p. 505). But contraction

cannot restore lost momentum.]

[Footnote 1162: _Stellar Evolution, and its Relations to Geological

Time_, 1889.]

[Footnote 1163: _Comptes Rendus_, t. lii., p. 481. See also Kirkwood,

_Observatory_, vol. iii., p. 409.]

[Footnote 1164: Fouché, _Comptes Rendus_, t. xcix., p. 903.]

[Footnote 1165: _Astroph. Jour._, vol. xiii., p. 338.]

[Footnote 1166: _Month. Not._, vol. xxix., p. 96.]

[Footnote 1167: _Pop. Astr._, p. 257.]

[Footnote 1168: _Sur l'Origine du Monde_, 1884.]

[Footnote 1169: Kirkwood adverted to it in 1864, _Am. Jour._, vol.

xxxviii., p. 1.]

[Footnote 1170: _Bull. Astr._, t. ii.]

[Footnote 1171: _Nature_, vol. xxxi., p. 506.]

[Footnote 1172: _Formation Mécanique du Système du Monde; Bull. Astr._,

t. xiv., p. 313 (O. Callandreau). See also, _Le Problème Solaire_, by

l'Abbé Th. Moreux, 1900.]

[Footnote 1173: _Phil. Trans._, vol. clxxi., p. 713.]

[Footnote 1174: Mr. J. Nolan has pointed out (_Nature_, vol. xxxiv., p.

287) that the length of the equal day and month will be reduced to about

1,240 hours by the effects of _solar_ tidal friction.]

[Footnote 1175: _Phil. Trans._, vol. clxxi., p. 835.]

[Footnote 1176: _Nature_, vol. xxxiii., p. 368; see also Nolan, _Ibid._,

vol. xxxiv., p. 286.]

[Footnote 1177: _Phil. Trans._, vol. clxxviii., p. 422.]

[Footnote 1178: _Ibid._, vol. clxxii., p. 491.]

[Footnote 1179: _Ibid._, p. 530.]

[Footnote 1180: _Satellite Evolution_, Melbourne, 1895; _Knowledge_,

vol. xviii., p. 205.]

[Footnote 1181: _Phil. Trans._, vol. clxxii., p. 533.]

[Footnote 1182: This was perceived by M. Ed. Roche in 1872. _Mém. de

l'Acad. des Sciences de Montpellier_, t. viii., p. 247.]

[Footnote 1183: _Nature_, vol. xxxiv., p. 287.]

[Footnote 1184: _Bull. Astr._, t. ii., p. 223.]

[Footnote 1185: _Montpellier Méms._, t. viii., p. 242.]

[Footnote 1186: _Amer. Jour._, vol. xxxviii. (1864), p. 1.]

[Footnote 1187: Wolf, _Bull. Astr._, t. ii., p. 76.]

A Popular History of Astronomy During the Nineteenth Century Fourth Edition · 第 9 / 15 章