The authors call attention to the fact that the Sun's equator

is inclined at a small angle, 7 degrees, to the common planes

of the planetary system, and Chamberlin holds this to be one of

the strong points in favor of the planetesimal hypothesis. He

reasons thus: the star which passed close to our Sun and drew

out the planetary materials in the form of spiral streams must

have moved in the plane of the spiral; that is, in the plane of

our planetary system. Some of the materials would be drawn out

from our Sun only a very short distance and then fall back upon

the Sun. Great tidal waves would be formed on opposite sides of

the Sun, and these would try to follow the disturbing body. The

effect of these waves and of the materials which fall back

would be to change the Sun's original rotation plane in the

direction of the disturbing body's orbital plane.

Now the chance for a disturbing star's passing around our Sun

in a plane making a large angle, say from 45 degrees to 90

degrees, with the Sun's equator, is much greater than for a

small angle 0 degrees to 45 degrees. The chances are greatest

that the angle will be 90 degrees. Only those disturbing stars

which approach our Sun PRECISELY in the plane of the Sun's

equator could move around the Sun in this plane. All those

approaching along any line parallel to the Sun's equatorial

plane, but lying outside of this plane, and all those whose

directions of approach make any angle whatever with the

equatorial plane, would find it impossible to move in that

plane. That the angle under this hypothesis is only 7 degrees

is surprising, though, as we are dealing with but a single

case, we can not say, I think, that this militates either for

or against the hypothesis. We are entitled to say only that

unless the approach was so close as to cause disturbances in

our Sun to relatively great depths, the angle referred to would

have only one chance in ten or fifteen or twenty to be as small

as 7 degrees. Any disturbance which succeeded in taking out of

the Sun only 1/7 of 1 per cent. of its mass could scarcely

succeed in shifting the axis of rotation of the remaining 99

6/7 per cent. very much, I think. If the angle were 30 degrees

or 50 degrees or 80 degrees, instead of 7 degrees, the case for

the planetesimal hypothesis would be somewhat stronger.

A remarkable fact concerning the Sun is that the equatorial

region rotates once around in a shorter time than the regions

in higher latitudes require. The rotation period of the Sun's

equator is about 24 days; the period at latitude 45 degrees is

28 days; and at 75 degrees, 33 days. The planetesimal

hypothesis attributes this equatorial acceleration to the

falling back into the Sun of the materials which had been

lifted out to a short distance by the disturbing body, and to

the forward-rushing tide raised in the equatorial regions by

the disturbing body. This may well have occurred. However, we

must remember that the same phenomenon exists certainly in

Jupiter and Saturn, and quite probably in Uranus and Neptune;

that is, in all the bodies in the system that are gaseous and

free to show the effect. It seems to be the result of a

principle which has operated throughout the solar system, not

requiring, at least not directly requiring, the passage of a

disturbing star. I think the most plausible explanation of this

curious phenomenon is that great quantities of materials

originally revolving around the Sun and around each of the

planets have gradually been drawn into these bodies, by

preference into their equatorial areas. Such masses of matter

moving in orbits very close to these bodies must have traveled

with speeds vastly higher than the surface speeds of the

bodies. To illustrate, the rotational velocity of a particle

now in the Sun's surface at the equator is approximately 2 km.

per second. A small body revolving around the Sun close to his

surface, rapidly enough to prevent its falling quickly upon the

Sun, must have a velocity of more than 400 km. per second. If,

now, this small body encounters some resistance it will fall

into the Sun, and as it is traveling more than 200 times as

rapidly as the solar materials into which it drops, it will

both generate heat and accelerate the rotational velocity of

the surrounding materials. In the same way the equatorial

accelerations in Jupiter and Saturn can receive simple

explanation. The point is not necessarily in opposition to the

planetesimal hypothesis; but whatever the explanation, it ought

to apply to the planet as well as to the Sun.

If the spiral nebulae have been formed in accordance with

Chamberlin and Moulton's hypothesis, the secondary nuclei in

them must revolve in a great variety of elliptic orbits. The

orbits would intersect, and in the course of long ages the

separate masses would collide and combine and the number of

separate masses would constantly grow smaller. Moulton has

shown that IN GENERAL the combining of two masses whose orbits

intersect causes the combined mass to move in an orbit more

nearly circular than the average orbit of the separate masses,

and in general in orbit planes more nearly coincident with the

general plane of the system. Accordingly, the major planets

should move in orbits more nearly circular and more nearly in

the plane of the system than do the asteroids; and so they do.

If the asteroids should combine to form one planet the orbit of

this planet should be much less eccentric than the average of

all the present asteroid eccentricities, and the deviation of

its orbit plane should be less than the average deviation of

the present planes. We can not doubt that this would be the

case. Mercury and Mars, the smallest planets, should have,

according to this principle, the largest eccentricities and

orbital inclinations of any of the major planets. This is true

of the eccentricities, but Mars's orbit plane, contrarily, has

a small inclination. Venus and the Earth, next in size, should

have the next largest inclinations and eccentricities, but they

do not; Venus's eccentricity is the smallest of all. The

Earth's orbital inclination and eccentricity are both small.

Jupiter and Saturn, Uranus and Neptune, should have the

smallest orbital inclinations; their average inclination is

about the same as for Venus and the Earth. They should likewise

have the smallest eccentricities. Neptune, the smallest of the

four, has an orbit nearly circular; Jupiter, Saturn and Uranus

have eccentricities more than 4 times those of Venus and the

Earth. Considering the four large planets as one group and the

four small planets as another group, we find that the

inclinations of the orbits of the two groups, per unit mass,

are about equal; but the average eccentricity of the orbits of

the large planets, per unit mass, is 21 times that of the

orbits of the small planets.[1] The evidence, except as to the

asteroids and Mercury, is not favorable to the planetesimal

hypothesis, unless we make special assumptions as to the

distribution of materials in the spiral nebulae.

[2] The average eccentricity of the orbits of the four inner

planets (per unit mass) is 0.0221, and of the four outer

planets is 0.0489.

The fact that the disturbing body drew 225 times as much matter

a great distance to form the four large planets as it drew out

a short distance to form the four small planets and the

asteroids seems difficult of explanation on the planetesimal

hypothesis. However, this distribution of matter is at present

a difficulty in any of the hypotheses. The planetesimal

hypothesis explains well all west to east rotations of the

planets on their axes, but to make Uranus rotate nearly at

right angles to the plane of the system, and Neptune in a plane

inclined 135 degrees to the plane of the system, is a

difficulty in any of the hypotheses, unless special assumptions

are made to fit each case.

The authors succeed well, I think, in showing that the

satellites should prefer to revolve around their planets in the

direction of the planetary revolution and rotation, especially

for close satellites, and, on the basis of special assumptions,

in the reverse direction for satellites at a greater distance.

They show that the chances favor small eccentricities for

satellites revolving about their planets in the west to east,

or direct sense, and large eccentricities for satellites moving

in retrograde directions. The inner satellite of Mars and the

rings of Saturn make no special difficulty under the

planetesimal hypothesis.

The evidence of the comets, as bona fide members of the solar

system which approach the Sun almost, and perhaps quite,

indifferently from all directions, is that the volume of space

occupied by the parent structure of the system was of enormous

dimensions, both at right angles to the present principal plane

of the system and in that plane. We are accustomed to think of

the spiral nebulae as thin relatively to their major diameters.

To this extent the planetesimal hypothesis does not furnish a

good explanation of the origin of comets, unless we assume that

a small amount of matter was widely scattered in all directions

around the parent spiral; and this conception leads to some

apparent difficulties. The origin of the comets is difficult to

explain under any of the hypotheses.

RESUME OF HYPOTHESES

Kant's hypothesis had the great defect of trying to prove too

much. It started from matter AT REST, and came to grief in

trying to give a motion of rotation to the entire mass through

the operation of internal forces alone--an impossibility.

Kant's idea of nuclei or centers of gravitational attraction,

scattered here and there throughout the chaotic mass, which

grew into the planets and their satellites, is very valuable.

Laplace's hypothesis had the great advantage of starting with

an extended mass already in rotation, but it violated fatally

the law of constancy of moment of momentum. We should expect

this hypothesis to create a solar system free from

irregularities, very much as if it were the product of an

instrument-maker's precision lathe. The solar system as it

exists is a combination of regularities and many surprising

irregularities.

Chamberlin and Moulton's hypothesis has the advantage of a

parent mass in rotation, practically in a common plane, and

with the materials distributed at distances from the nucleus as

nearly in harmony with the known distribution of matter in the

solar system as we care to have them, except perhaps as to the

comets. In effect it retains all the advantageous qualities of

Kant's proposals. It seems to have the flexibility required in

meeting the irregularities that we see in our system.

CONCERNING THE ORIGIN OF SPIRAL NEBULAE

I think it is very doubtful whether the spiral nebulae have in

general been formed by the close approaches of pairs of stars,

as the authors have postulated for the assumed solar spiral.[2]

The distribution of the spirals seems to me to negative the

idea. To witness the close approach of two stars we must look

in the direction where the stars are. To the best of

present-day knowledge the stars are in a spheroid whose longer

axes are coincident with the plane of the Milky Way. If this is

so, the close approach of pairs of stars should occur

preeminently in the Milky Way, and we should find the spirals

prevailingly in and near the Milky Way. This is precisely where

we do not find them. In fact, they seem to abhor the Milky Way.

The new stars, which are credibly explained as the products of

collisions of stars with nebulae, are found preeminently in the

Milky Way and almost negligibly in the regions outside of the

Milky Way. Again, the spirals are believed to be, on the whole,

of enormous size. They are too far away to let us measure their

distances by the usual methods, and they move too slowly on the

surface of the sphere to have let us determine their proper

motions. Slipher's recent work with a spectrograph seems to

show that the dozen spirals observed by him are moving with

high speeds of approach and recession; from 300 km. per second

approach in the case of the Andromeda nebula to 1,100 km. per

second recession in the case of several objects. If the spirals

are moving at random their speeds at right angles to the line

of sight must be even greater than their speeds of approach and

recession. Unless they are very distant bodies their proper

motions should be detected by observations extending over only

a few years. My colleague Curtis has this year compared recent

photographs of some 25 spirals with photographs of the same

object made by Keeler fifteen years ago. They reveal no

appreciable proper motions, or rotations. In this same interval

Neptune has revolved more than 30 degrees. Slipher has recently

measured the rotational speed of one "spindle" nebula, believed

to be a spiral. He finds it to be enormously rapid; no motions

in the solar system approach it in magnitude. The evidence is

to the effect that the spirals are in general very far away;[3]

perhaps on or beyond the confines of our stellar system, but

not certainly so. Accordingly, we are led to believe that the

spirals studied thus far have diameters 20 times or 100 times,

or in some cases several thousand times, the diameter of our

solar system. It is difficult to avoid the conclusion that in

general they are immensely more massive than is our solar

system. The spiral which has been assumed as the forerunner of

our system must have been of diminutive size as compared with

the larger and brighter spirals which we see to-day.

[2] It would seem that all rotating nebulae should in reality

possess some of the attributes of spiral motion. Whether the

spiral structure should be visible or invisible to a

terrestrial observer would depend upon the sizes and distances

of the nebulae, upon the distribution of materials composing

them, and perhaps upon other factors. See developed the

hypothesis that spiral nebulae owe their origin to the

collision of two nebulae. Collisions of this kind could readily

occur because of the enormous dimensions of the nebulae, and

motions of rotation and consequently spiral structure might

readily result therefrom. The abnormally high speeds of the

spiral nebulae are apparently a very strong objection to the

hypothesis.

[3] Bohlin found a parallax of 0"17 for the Andromeda Nebula,

and Lampland thinks that Nebula N.G.G. 4594 has a proper motion

of approximately 0"05 per annum.

We are sadly in need of information concerning the constitution

of the spiral nebulae. Their spectra appear to be prevailingly

of the solar type, except that a very small proportion contain

some bright lines in addition to the continuous spectrum. So

far as their spectra are concerned, they may be great clusters

of stars, or they may consist each of a central star sending

its light out upon surrounding dark materials and thus

rendering these materials visible to us. The first alternative

is unsatisfactory, for all parts of spirals have hazy borders,

as if the structure is nebulous or consists of irregular groups

of small masses; and the second alternative is unsatisfactory,

for in many spirals the most outlying masses seem to be as

bright as masses of the same areas situated only one half as

far from the center, whereas in general the inner area should

be at least four times as bright as the outer area. All

astronomers are ready to confess that we do not know much about

the conditions existing in spiral nebulae.

THE EARTH-MOON SYSTEM

Our Earth and Moon form a unique combination in that they are

more nearly of the same size than are any other planet and its

satellites in our system. It required a 26-inch telescope on

the Earth to discover the tiny moons of Mars; but an astronomer

on Mars does not need any telescope to see the Earth and Moon

as a double planet--the only double planet in the solar system.

According to the Kantian school of hypotheses the Earth and

Moon owe their unique character to the accident that two

centers of condensation--two nuclei--not very unequal in mass,

were formed close to each other and were endowed with or

acquired motions such that they revolved around each other.

They drew in the surrounding materials; one of the two bodies

got somewhat the advantage of the other in gravitational

attraction; it succeeded in building itself up more than the

other nucleus did; and the Earth and the Moon were the result.

According to the Laplacean hypothesis, on the contrary, the

Earth and Moon were originally one body, gaseous and in

rotation. This ball of gas radiated heat, diminished in size,

rotated more and more rapidly, and finally abandoned a ring of

nebulosity, which later broke up and eventually condensed into

one mass called the Moon. The central mass composed the Earth.

It is a curious fact that Venus, which is only a shade smaller

than the Earth, should not have divided into two bodies

comparable with the Earth and Moon. Have the tides on Venus

produced by the Sun always been strong enough to keep the

rotation and revolution periods equal, as they are thought to

be now, and thus to have given no opportunity for a rapidly

rotating Venus to divide into two masses?

A third hypothesis of the Moon's origin is due principally to

Darwin. He and Poincare have shown that a great rotating mass

of fluid matter, such as the Earth-Moon could be assumed to

have been, by cooling, contracting and increasing rotation

speed, would, under certain conditions thought to be

reasonable, become unstable and eventually divide into two

bodies revolving around their common center of mass, at first

with their surfaces nearly in contact. Here would begin to act

a tide-raising force which must have played, according to

Darwin's deductions, a most important part in the further

history of the Earth and Moon. The Earth would produce enormous

tides in the Moon, and the Moon much smaller tides in the

Earth. Both bodies would contract in size, through loss of

heat, and would try to rotate more and more rapidly. The two

rotating bodies would try to carry the matter in the tidal

waves around with the rest of the materials in the bodies, but

the pull of each body upon the wave materials in the other

would tend to slow down the speed of rotation. The tidal

resistance to rotation would be slight if the bodies at any

time were attenuated gaseous masses, for the friction within

the surface strata would be slight. Nevertheless, there would

eventually be a gradual slowing down of the Moon's rotation, a

gradual slowing down of the Earth's rotation, and a slow

increase in the distance between the two bodies. In other

words, the Moon's day, the Earth's day and our month would

gradually increase in length. Carried to its logical

conclusion, the Moon would eventually turn the same face to the

Earth, the Earth would eventually turn the same face to the

Moon, and the Earth's day and the Moon's day would equal the

month in length. The central idea in this logic is as old as

Kant: in 1754 he published an important paper in which he said

that tidal interactions between Earth and Moon had caused the

Moon to keep the same face turned toward us, that the Earth's

day was being very slowly lengthened, and that our planet would

eventually turn the same face to the Moon. Laplace, a

half-century later, proposed the action of such a force in

connection with the explanation of lunar phenomena, and

Helmholtz, just 100 years after Kant's paper was published,

lent his support to this principle; but Sir George Darwin has

been the great contributor to the subject. His popular volume,

"The Tides," devotes several chapters to the effects of tidal

friction upon the motions of two bodies in mutual revolution.

We must pass over the difficult and complicated intermediate

steps to Darwin's conclusions concerning the Earth and Moon,

which are substantially as follows: the Earth and Moon were

originally much closer together than they now are: after a very

long period of time, amounting to hundreds of millions of

years, the Moon will revolve around the Earth in 55 days

instead of in 27 days as at present; and the Moon and Earth

will then present the same faces constantly to each other. The

estimated period of time required, and the final length of day

and month, 55 days, are of course not insisted upon as accurate

by Darwin.

These tidal forces were unavoidably active, it matters not if

the Earth and Moon were originally one body, as Laplace and

Darwin have postulated, or originally two bodies, growing up

from two nuclei, in accordance with the Kantian school. Whether

these forces have been sufficiently strong to have brought the

Earth and Moon to their present relation, or will eventually

equalize the Moon's day, the Earth's day, and the month, is a

vastly more difficult question. Moulton's researches have cast

serious doubt upon this conclusion. All such investigations are

enormously difficult, and many questionable assumptions must be

made if we seek to go back to the Moon's origin, or forward to

its ultimate destiny.

Tidal waves, in order to be effective in reducing the

rotational speed of a planet, must be accompanied by internal

friction; and this requires that the planet be to some extent

inelastic. It was the view of Darwin and others that the

viscous state of the Earth and Moon permitted wave friction to

come into play. Michelson has recently proved that the Earth

has a high degree of elasticity. It deforms in response to

tidal forces, but quickly recovers from the action of these

forces. It therefore seems that the rate of tidal evolution of

the Earth-Moon system at present and in the future must be

extremely slow, and possibly almost negligible. What the

conditions within the Earth and Moon were in the distant past

is uncertain, but these bodies probably passed through viscous

stages which endured through enormously long periods of time.

No one seriously doubts that Jupiter, Saturn, Uranus and

Neptune are now largely gaseous, and that they will evolve,

through various degrees of viscosity, into the solid and

comparatively elastic state. It is natural to assume that the

Earth has already passed through an analogous experience.

The Moon turns always the same hemisphere toward the Earth.

Observations of Venus and Mercury are prevailingly to the

effect that those planets always turn the same hemispheres

toward the Sun. Many, and perhaps all, of the satellites of

Jupiter and Saturn seem to turn the same hemispheres always

toward their respective planets. This widely prevailing

phenomenon is no doubt due to a widely prevailing cause, which

astronomers have all but unanimously attributed to tidal

action.

BINARY STAR SYSTEMS

That an original mass actually divided to form the Earth and

Moon, according to the Laplacian or the Darwin-Poincare

principle, seems to be extremely doubtful, especially on

account of their diminutive sizes, and I greatly prefer to

think that the Earth and Moon were built up from two nuclei;

but that very much greater masses, masses larger on the average

than our Sun, composing highly attenuated stars, have divided

each into two masses to form many or most of our double stars,

I firmly believe. The two component stars would in such a case

at first revolve around each other with their surfaces almost

or quite in contact. Tidal forces would very gradually cause

the bodies to move in orbits of larger and larger size, with

correspondingly longer periods of revolutions, and the orbits

would become constantly more eccentric. While these processes

were under way the component bodies would be radiating heat and

growing smaller, and their spectra would be changing into the

more advanced types. We can not hope to watch such changes as

they occur, but we can, I think, find abundant illustrations of

these processes in the double stars. I have given reasons for

believing that one star in every two and one half, as a minimum

proportion, is not the single star which it appears to be to

the eye or in the telescope, but is a system of two or more

suns in mutual revolution. The formation of double stars,

therefore, is not a sporadic process: it is one of the

straightforward results of the evolutionary process.

The Scientific Monthly, October to December, 1915 · 第 24 / 30 段