CHAPTER II

MERCURY, A WORLD OF TWO FACES AND MANY CONTRASTS

Mercury, the first of the other worlds that we are going to consider,

fascinates by its grotesqueness, like a piece of Chinese ivory carving,

so small is it for its kind and so finished in its eccentric details. In

a little while we shall see how singular Mercury is in many of the

particulars of planetary existence, but first of all let us endeavor to

obtain a clear idea of the actual size and mass of this strange little

planet. Compared with the earth it is so diminutive that it looks as if

it had been cut out on the pattern of a satellite rather than that of an

independent planet. Its diameter, 3,000 miles, only exceeds the moon's

by less than one half, while both Jupiter and Saturn, among their

remarkable collections of moons, have each at least one that is

considerably larger than the planet Mercury. But, insignificant though

it be in size, it holds the place of honor, nearest to the sun.

It was formerly thought that Mercury possessed a mass greatly in excess

of that which its size would seem to imply, and some estimates, based

upon the apparent effect of its attraction on comets, made it equal in

mean density to lead, or even to the metal mercury. This led to curious

speculations concerning its probable metallic composition, and the

possible existence of vast quantities of such heavy elements as gold in

the frame of the planet. But more recent, and probably more correct,

computations place Mercury third in the order of density among the

members of the solar system, the earth ranking as first and Venus as

second. Mercury's density is now believed to be less than the earth's in

the ratio of 85 to 100. Accepting this estimate, we find that the force

of gravity upon the surface of Mercury is only one third as great as

upon the surface of the earth--i.e., a body weighing 300 pounds on the

earth would weigh only 100 pounds on Mercury.

This is an important matter, because not only the weight of bodies, but

the density of the atmosphere and even the nature of its gaseous

constituents, are affected by the force of gravity, and if we could

journey from world to world, in our bodily form, it would make a great

difference to us to find gravity considerably greater or less upon other

planets than it is upon our own. This alone might suffice to render some

of the planets impossible places of abode for us, unless a decided

change were effected in our present physical organization.

One of the first questions that we should ask about a foreign world to

which we proposed to pay a visit, would relate to its atmosphere. We

should wish to know in advance if it had air and water, and in what

proportions and quantities. However its own peculiar inhabitants might

be supposed able to dispense with these things, to _us_ their presence

would be essential, and if we did not find them, even a planet that

blazed with gold and diamonds only waiting to be seized would remain

perfectly safe from our invasion. Now, in the case of Mercury, some

doubt on this point exists.

Messrs. Huggins, Vogel, and others have believed that they found

spectroscopic proof of the existence of both air and the vapor of water

on Mercury. But the necessary observations are of a very delicate

nature, and difficult to make, and some astronomers doubt whether we

possess sufficient proof that Mercury has an atmosphere. At any rate,

its atmosphere is very rare as compared with the earth's, but we need

not, on that account, conclude that Mercury is lifeless. Possibly, in

view of certain other peculiarities soon to be explained, a rare

atmosphere would be decidedly advantageous.

Being much nearer the sun than the earth is, Mercury can be seen by us

only in the same quarter of the sky where the sun itself appears. As it

revolves in its orbit about the sun it is visible, alternately, in the

evening for a short time after sunset and in the morning for a short

time before sunrise, but it can never be seen, as the outer planets are

seen, in the mid-heaven or late at night. When seen low in the twilight,

at evening or morning, it glows with the brilliance of a bright

first-magnitude star, and is a beautiful object, though few casual

watchers of the stars ever catch sight of it. When it is nearest the

earth and is about to pass between the earth and the sun, it temporarily

disappears in the glare of the sunlight; and likewise, when it it is

farthest from the earth and passing around in its orbit on the opposite

side of the sun, it is concealed by the blinding solar rays.

Consequently, except with the instruments of an observatory, which are

able to show it in broad day, Mercury is never visible save during the

comparatively brief periods of time when it is near its greatest

apparent distance east or west from the sun.

The nearer a planet is to the sun the more rapidly it is compelled to

move in its orbit, and Mercury, being the nearest to the sun of all the

planets, is by far the swiftest footed among them. But its velocity is

subject to remarkable variation, owing to the peculiar form of the orbit

in which the planet travels. This is more eccentric than the orbit of

any other planet, except some of the asteroids. The sun being situated

in one focus of the elliptical orbit, when Mercury is at perihelion, or

nearest to the sun, its distance from that body is 28,500,000 miles, but

when it is at aphelion, or farthest from the sun, its distance is

43,500,000 miles. The difference is no less than 14,000,000 miles! When

nearest the sun Mercury darts forward in its orbit at the rate of

twenty-nine miles in a second, while when farthest from the sun the

speed is reduced to twenty-three miles.

Now, let us return for a moment to the consideration of the wonderful

variations in Mercury's distance from the sun, for we shall find that

their effects are absolutely startling, and that they alone suffice to

mark a wide difference between Mercury and the earth, considered as the

abodes of sentient creatures. The total change of distance amounts, as

already remarked, to 14,000,000 miles, which is almost half the entire

distance separating the planet from the sun at perihelion. This immense

variation of distance is emphasized by the rapidity with which it takes

place. Mercury's periodic time, i.e., the period required for it to make

a single revolution about the sun--or, in other words, the length of its

year--is eighty-eight of our days. In just one half of that time, or in

about six weeks, it passes from aphelion to perihelion; that is to say,

in six weeks the whole change in its distance from the sun takes place.

In six weeks Mercury falls 14,000,000 miles--for it _is_ a fall, though

in a curve instead of a straight line--falls 14,000,000 miles toward the

sun! And, as it falls, like any other falling body it gains in speed,

until, having reached the perihelion point, its terrific velocity

counteracts its approach and it begins to recede. At the end of the next

six weeks it once more attains its greatest distance, and turns again to

plunge sunward.

Of course it may be said of every planet having an elliptical orbit

that between aphelion and perihelion it is falling toward the sun, but

no other planet than Mercury travels in an orbit sufficiently eccentric,

and approaches sufficiently near to the sun, to give to the mind so

vivid an impression of an actual, stupendous fall!

Next let us consider the effects of this rapid fall, or approach, toward

the sun, which is so foreign to our terrestrial experience, and so

appalling to the imagination.

First, we must remember that the nearer a planet is to the sun the

greater is the amount of heat and light that it receives, the variation

being proportional to the inverse square of the distance. The earth's

distance from the sun being 93,000,000 miles, while Mercury's is only

36,000,000, it follows, to begin with, that Mercury gets, on the

average, more than six and a half times as much heat from the sun as the

earth does. That alone is enough to make it seem impossible that Mercury

can be the home of living forms resembling those of the earth, for

imagine the heat of the sun in the middle of a summer's day increased

six or seven fold! If there were no mitigating influences, the face of

the earth would shrivel as in the blast of a furnace, the very stones

would become incandescent, and the oceans would turn into steam.

Still, notwithstanding the tremendous heat poured upon Mercury as

compared with that which our planet receives, we can possibly, and for

the sake of a clearer understanding of the effects of the varying

distance, which is the object of our present inquiry, find a loophole to

admit the chance that yet there may be living beings there. We might,

for instance, suppose that, owing to the rarity of its atmosphere, the

excessive heat was quickly radiated away, or that there was something in

the constitution of the atmosphere that greatly modified the effective

temperature of the sun's rays. But, having satisfied our imagination on

this point, and placed our supposititious inhabitants in the hot world

of Mercury, how are we going to meet the conditions imposed by the

rapid changes of distance--the swift fall of the planet toward the sun,

followed by the equally swift rush away from it? For change of distance

implies change of heat and temperature.

It is true that we have a slight effect of this kind on the earth.

Between midsummer (of the northern hemisphere) and midwinter our planet

draws 3,000,000 miles nearer the sun, but the change occupies six

months, and, at the earth's great average distance, the effect of this

change is too slight to be ordinarily observable, and only the

astronomer is aware of the consequent increase in the apparent size of

the sun. It is not to this variation of the sun's distance, but rather

to the changes of the seasons, depending on the inclination of the

earth's axis, that we owe the differences of temperature that we

experience. In other words, the total supply of heat from the sun is not

far from uniform at all times of the year, and the variations of

temperature depend upon the distribution of that supply between the

northern and southern hemispheres, which are alternately inclined

sunward.

But on Mercury the supply of solar heat is itself variable to an

enormous extent. In six weeks, as we have seen, Mercury diminishes its

distance from the sun about one third, which is proportionally ten times

as great a change of distance as the earth experiences in six months.

The inhabitants of Mercury in those six pregnant weeks see the sun

expand in the sky to more than two and a half times its former

magnitude, while the solar heat poured upon them swiftly augments from

something more than four and a half times to above eleven times the

amount received upon the earth! Then, immediately, the retreat of the

planet begins, the sun visibly shrinks, as a receding balloon becomes

smaller in the eyes of its watchers, the heat falls off as rapidly as it

had previously increased, until, the aphelion point being reached, the

process is again reversed. And thus it goes on unceasingly, the sun

growing and diminishing in the sky, and the heat increasing and

decreasing by enormous amounts with astonishing rapidity. It is

difficult to imagine any way in which atmospheric influences could

equalize the effects of such violent changes, or any adjustments in the

physical organization of living beings that could make such changes

endurable.

But we have only just begun the story of Mercury's peculiarities. We

come next to an even more remarkable contrast between that planet and

our own. During the Paris Exposition of 1889 a little company of

astronomers was assembled at the Juvisy observatory of M. Flammarion,

near the French capital, listening to one of the most surprising

disclosures of a secret of nature that any _savant_ ever confided to a

few trustworthy friends while awaiting a suitable time to make it

public. It was a secret as full of significance as that which Galileo

concealed for a time in his celebrated anagram, which, when at length he

furnished the key, still remained a riddle, for then it read: "The

Mother of the Loves imitates the Shapes of Cynthia," meaning that the

planet Venus, when viewed with a telescope, shows phases like those of

the moon. The secret imparted in confidence to the knot of astronomers

at Juvisy came from a countryman of Galileo's, Signor G. V.

Schiaparelli, the Director of the Observatory of Milan, and its purport

was that the planet Mercury always keeps the same face directed toward

the sun. Schiaparelli had satisfied himself, by a careful series of

observations, of the truth of his strange announcement, but before

giving it to the world he determined to make doubly sure. Early in 1890

he withdrew the pledge of secrecy from his friends and published his

discovery.

No one can wonder that the statement was generally received with

incredulity, for it was in direct contradiction to the conclusions of

other astronomers, who had long believed that Mercury rotated on its

axis in a period closely corresponding with that of the earth's

rotation--that is to say, once every twenty-four hours. Schiaparelli's

discovery, if it were received as correct, would put Mercury, as a

planet, in a class by itself, and would distinguish it by a peculiarity

which had always been recognized as a special feature of the moon, viz.,

that of rotating on its axis in the same period of time required to

perform a revolution in its orbit, and, while this seemed natural enough

for a satellite, almost nobody was prepared for the ascription of such

eccentric conduct to a planet.

The Italian astronomer based his discovery upon the observation that

certain markings visible on the disk of Mercury remained in such a

position with reference to the direction of the sun as to prove that the

planet's rotation was extremely slow, and he finally satisfied himself

that there was but one rotation in the course of a revolution about the

sun. That, of course, means that one side of Mercury always faces toward

the sun while the opposite side always faces away from it, and neither

side experiences the alternation of day and night, one having perpetual

day and the other perpetual night. The older observations, from which

had been deduced the long accepted opinion that Mercury rotated, like

the earth, once in about twenty-four hours, had also been made upon the

markings on the planet's disk, but these are not easily seen, and their

appearances had evidently been misinterpreted.

The very fact of the difficulty of seeing any details on Mercury tended

to prevent or delay corroboration of Schiaparelli's discovery. But there

were two circumstances that contributed to the final acceptance of his

results. One of these was his well-known experience as an observer and

the high reputation that he enjoyed among astronomers, and the other was

the development by Prof. George Darwin of the theory of tidal friction

in its application to planetary evolution, for this furnished a

satisfactory explanation of the manner in which a body, situated as near

the sun as Mercury is, could have its axial rotation gradually reduced

by the tidal attraction of the sun until it coincided in period with its

orbital revolution.

Accepting the accuracy of Schiaparelli's discovery, which was

corroborated in every particular in 1896 by Percival Lowell in a special

series of observations on Mercury made with his 24-inch telescope at

Flagstaff, Arizona, and which has also been corroborated by others, we

see at once how important is its bearing on the habitability of the

planet. It adds another difficulty to that offered by the remarkable

changes of distance from the sun, and consequent variations of heat,

which we have already discussed. In order to bring the situation home to

our experience, let us, for a moment, imagine the earth fallen into

Mercury's dilemma. There would then be no succession of day and night,

such as we at present enjoy, and upon which not alone our comfort but

perhaps our very existence depends, but, instead, one side of our

globe--it might be the Asiatic or the American half--would be

continually in the sunlight, and the other side would lie buried in

endless night. And this condition, so suggestive of the play of pure

imagination, this plight of being a two-faced world, like the god

Janus, one face light and the other face dark, must be the actual state

of things on Mercury.

There is one interesting qualification. In the case just imagined for

the earth, supposing it to retain the present inclination of its axis

while parting with its differential rotation, there would be an

interchange of day and night once a year in the polar regions. On

Mercury, whose axis appears to be perpendicular, a similar phenomenon,

affecting not the polar regions but the eastern and western sides of the

planet, is produced by the extraordinary eccentricity of its orbit. As

the planet alternately approaches and recedes from the sun its orbital

velocity, as we have already remarked, varies between the limits of

twenty-three and thirty-five miles per second, being most rapid at the

point nearest the sun. But this variation in the speed of its revolution

about the sun does not, in any manner, affect the rate of rotation on

its axis. The latter is perfectly uniform and just fast enough to

complete one axial turn in the course of a single revolution about the

sun. The accompanying figure may assist the explanation.

[Illustration: DIAGRAM SHOWING THAT, OWING TO THE ECCENTRICITY OF ITS

ORBIT, AND ITS VARYING VELOCITY, MERCURY, ALTHOUGH MAKING BUT ONE TURN

ON ITS AXIS IN THE COURSE OF A REVOLUTION ABOUT THE SUN, NEVERTHELESS

EXPERIENCES ON PARTS OF ITS SURFACE THE ALTERNATION OF DAY AND NIGHT.]

Let us start with Mercury in perihelion at the point _A_. The little

cross on the planet stands exactly under the sun and in the center of

the illuminated hemisphere. The large arrows show the direction in which

the planet travels in its revolution about the sun, and the small curved

arrows the direction in which it rotates on its axis. Now, in moving

along its orbit from _A_ to _B_ the planet, partly because of its

swifter motion when near the sun, and partly because of the elliptical

nature of the orbit, traverses a greater angular interval with reference

to the sun than the cross, moving with the uniform rotation of the

planet on its axis, is able to traverse in the same time. As drawn in

the diagram, the cross has moved through exactly ninety degrees, or one

right angle, while the planet in its orbit has moved through

considerably more than a right angle. In consequence of this gain of the

angle of revolution upon the angle of rotation, the cross at _B_ is no

longer exactly under the sun, nor in the center of the illuminated

hemisphere. It appears to have shifted its position toward the west,

while the hemispherical cap of sunshine has slipped eastward over the

globe of the planet.

In the next following section of the orbit the planet rotates through

another right angle, but, owing to increased distance from the sun, the

motion in the orbit now becomes slower until, when the planet arrives at

aphelion, _C_, the angular difference disappears and the cross is once

more just under the sun. On returning from aphelion to perihelion the

same phenomena recur in reverse order and the line between day and night

on the planet first shifts westward, attaining its limit in that respect

at _D_, and then, at perihelion, returns to its original position.

Now, if we could stand on the sunward hemisphere of Mercury what, to our

eyes, would be the effect of this shifting of the sun's position with

regard to a fixed point on the planet's surface? Manifestly it would

cause the sun to describe a great arc in the sky, swinging to and fro,

in an east and west line, like a pendulum bob, the angular extent of the

swing being a little more than forty-seven degrees, and the time

required for the sun to pass from its extreme eastern to its extreme

western position and back again being eighty-eight days. But, owing to

the eccentricity of the orbit, the sun swings much faster toward the

east than toward the west, the eastward motion occupying about

thirty-seven days and the westward motion about fifty-one days.

[Illustration: THE REGIONS OF PERPETUAL DAY, PERPETUAL NIGHT, AND

ALTERNATE DAY AND NIGHT ON MERCURY. IN THE LEFT-HAND VIEW THE OBSERVER

LOOKS AT THE PLANET IN THE PLANE OF ITS EQUATOR; IN THE RIGHT-HAND VIEW

HE LOOKS DOWN ON ITS NORTH POLE.]

Another effect of the libratory motion of the sun as seen from Mercury

is represented in the next figure, where we have a view of the planet

showing both the day and the night hemisphere, and where we see that

between the two there is a region upon which the sun rises and sets once

every eighty-eight days. There are, in reality, two of these lune-shaped

regions, one at the east and the other at the west, each between 1,200

and 1,300 miles broad at the equator. At the sunward edge of these

regions, once in eighty-eight days, or once in a Mercurial year, the sun

rises to an elevation of forty-seven degrees, and then descends again

straight to the horizon from which it rose; at the nightward edge, once

in eighty-eight days, the sun peeps above the horizon and quickly sinks

from sight again. The result is that, neglecting the effects of

atmospheric refraction, which would tend to expand the borders of the

domain of sunlight, about one quarter of the entire surface of Mercury

is, with regard to day and night, in a condition resembling that of our

polar regions, where there is but one day and one night in the course of

a year--and on Mercury a year is eighty-eight days. One half of the

remaining three quarters of the planet's surface is bathed in perpetual

sunshine and the other half is a region of eternal night.

And now again, what of life in such a world as that? On the night side,

where no sunshine ever penetrates, the temperature must be extremely

low, hardly greater than the fearful cold of open space, unless

modifying influences beyond our ken exist. It is certain that if life

flourishes there, it must be in such forms as can endure continual

darkness and excessive cold. Some heat would be carried around by

atmospheric circulation from the sunward side, but not enough, it would

seem, to keep water from being perpetually frozen, or the ground from

being baked with unrelaxing frost. It is for the imagination to picture

underground dwellings, artificial sources of heat, and living forms

suited to unearthlike environment.

What would be the mental effects of perpetual night upon a race of

intelligent creatures doomed to that condition? Perhaps not quite so

grievous as we are apt to think. The constellations in all their

splendor would circle before their eyes with the revolution of their

planet about the sun, and with the exception of the sun itself--which

they could see by making a journey to the opposite hemisphere--all the

members of the solar system would pass in succession through their

mid-heaven, and two of them would present themselves with a magnificence

of planetary display unknown on the earth. Venus, when in opposition

under the most favorable circumstances, is scarcely more than 24,000,000

miles from Mercury, and, showing herself at such times with a fully

illuminated disk--as, owing to her position within the orbit of the

earth, she never can do when at her least distance from us--she must be

a phenomenon of unparalleled beauty, at least four times brighter than

we ever see her, and capable, of course, of casting a strong shadow.

The earth, also, is a splendid star in the midnight sky of Mercury, and

the moon may be visible to the naked eye as a little attendant circling

about its brilliant master. The outer planets are slightly less

conspicuous than they are to us, owing to increase of distance.

The revolution of the heavens as seen from the night side of Mercury is

quite different in period from that which we are accustomed to, although

the apparent motion is in the same direction, viz., from east to west.

The same constellations remain above the horizon for weeks at a time,

slowly moving westward, with the planets drifting yet more slowly, but

at different rates, among them; the nearer planets, Venus and the earth,

showing the most decided tendency to loiter behind the stars.

On the side where eternal sunlight shines the sky of Mercury contains no

stars. Forever the pitiless blaze of day; forever,

"All in a hot and copper sky

The bloody sun at noon."

As it is difficult to understand how water can exist on the night

hemisphere, except in the shape of perpetual snow and ice, so it is

hard to imagine that on the day hemisphere water can ever be

precipitated from the vaporous form. In truth, there can be very little

water on Mercury even in the form of vapor, else the spectroscope would

have given unquestionable evidence of its presence. Those who think that

Mercury is entirely waterless and almost, if not quite, airless may be

right. In these respects it would then resemble the moon, and, according

to some observers, it possesses another characteristic lunar feature in

the roughening of its surface by what seem to be innumerable volcanic

craters.

But if we suppose Mercury to possess an atmosphere much rarer than that

of the earth, we may perceive therein a possible provision against the

excessive solar heat to which it is subjected, since, as we see on high

mountains, a light air permits a ready radiation of heat, which does not

become stored up as in a denser atmosphere.

As the sun pours its heat without cessation upon the day hemisphere the

warmed air must rise and flow off on all sides into the night

hemisphere, while cold air rushes in below, to take its place, from the

region of frost and darkness. The intermediate areas, which see the sun

part of the time, as explained above, are perhaps the scene of

contending winds and tempests, where the moisture, if there be any, is

precipitated, through the rapid cooling of the air, in whelming floods

and wild snow-storms driven by hurrying blasts from the realm of endless

night.

Enough seems now to have been said to indicate clearly the hopelessness

of looking for any analogies between Mercury and the earth which would

warrant the conclusion that the former planet is capable of supporting

inhabitants or forms of life resembling those that swarm upon the

latter. If we would still believe that Mercury is a habitable globe we

must depend entirely upon the imagination for pictures of creatures able

to endure its extremes of heat and cold, of light and darkness, of

instability, swift vicissitude, and violent contrast.

In the next chapter we shall study a more peaceful and even-going world,

yet one of great brilliancy, which possesses some remarkable

resemblances to the earth, as well as some surprising divergences from

it.

Other Worlds Their Nature, Possibilities and Habitability in the Light of the Latest Discoveries · 第 2 / 9 章