CHAPTER V

THE MOON

The Sun and Moon offer to our sight almost exactly the same apparent

diameters; to the eye, they look the same size. But as we know the Sun to

be 400 times as distant as the Moon, it is necessarily 400 times as large;

its surface must exceed that of the Moon by the square of 400, or 160,000;

its volume by the cube of 400, or 64,000,000. As the Sun is of low mean

density, its mass does not exceed that of the Moon in quite the same high

ratio; but it is equal in mass to

27,000,000 moons.

Compared with the Sun, the Moon is therefore an insignificant little

ball--a mere particle; but as a world for habitation it possesses some

advantages over the Sun. The first glance at it in a telescope is

sufficient to assure the observer that he is looking at a solid,

substantial globe. It is not only substantial, it is rugged; its surface

is broken up into mountains, hills, valleys, and plains; the mountains

stand out in sensible relief; it looks like a ball of solid silver boldly

embossed and chased.

So far all is to the good for the purpose of habitation. Wherever men

are, they must have a solid platform on which to stand; they must have a

stable terrene whereon their food may grow, and this the Moon could

supply. "The Earth's gloom of iron substance" is necessary for man here,

and the Moon appears to offer a like stability.

Another favourable condition is that we know that the Moon receives from

the Sun a sufficient supply of light and heat. Each square yard of its

surface receives, on the average, the same amount of light and heat that

would fall upon a square yard on the Earth that was presented towards the

Sun at the same inclination; and we know from our own experience that this

is sufficient for the maintenance of life.

And the Moon is near enough for us to subject her to a searching scrutiny.

Every part of the hemisphere turned toward us has been repeatedly

examined, measured, and photographed; to that extent our knowledge of its

topography is more complete than of the world on which we live. There are

no unexplored regions on our side of the Moon. The great photographs taken

in recent years at the observatories of Paris and of the University of

Chicago have shown thousands of "crater-pits," not more than a mile

across; and narrow lines on the Moon's surface have been detected with a

breadth less than one-tenth of this. An elevation on the Moon, if it rose

up abruptly from an open plain, would make its presence apparent by the

shadow which it would cast soon after sunrise or near sunset; in this way

an isolated building, if it were as large as the great pyramid of Ghizeh,

would also show itself, and all our great towns and cities would be

apparent as areas of indistinct mottling, though the details of the cities

would not be made out.

But if vegetation took the same forms on the Moon as on the Earth, and

passed through the same changes, we should have no difficulty in

perceiving the evidence of its presence. If we were transported to the

Moon and turned our eyes earthward, we should not need the assistance of

any telescope in order to detect terrestrial changes which would be

plainly connected with the seasonal changes of vegetation. The Earth would

present to us a disc four times the apparent diameter of the Moon, and on

that disc Canada would offer as great an area as the whole of the Moon

does to us. We could easily follow with the naked eye the change from the

glittering whiteness of the aspect of Canada when snow-covered in winter,

to the brown, green and gold which would succeed each other during the

brighter months of the year. And this type of change would alternate

between the northern and southern hemispheres, for the winter of Canada is

the summer of the Argentine, and conversely.

We ought, therefore, to have no difficulty in observing seasonal changes

on the Moon, if such take place. But nothing of the kind has ever been

remarked; no changes sufficiently pronounced for us to be sure of them are

ever witnessed. Here and there some slight mutations have been suspected,

nearly all accomplishing their cycle in the course of a lunar day; so that

it is difficult to separate them from changes purely apparent, brought

about by the change in the incidence of the illumination.

The difference in appearance of a given area on the Moon when viewed under

a low Sun and when the Sun is on the meridian is very striking. In the

first case everything is in the boldest relief; the shadows are long and

intensely black; the whole area under examination in the telescope seems

as if it might be handled. Under the high Sun, the contrasts are gone; the

scenery appears flat, many of the large conspicuous markings are only

recognized with difficulty. Thus the terse remark of Maedler, "The full

Moon knows no Maginus," has become a proverb amongst selenographers; yet

Maginus is a fine walled plain some eighty miles in diameter, and its

rampart attains a height in parts of 14,000 feet. Maginus lies near Tycho,

which has been well named "the lunar metropolis," for from it radiates the

principal system of bright streaks conspicuous on the full Moon. These

white streaks appear when the shadows have vanished or are growing short;

they are not seen under a low Sun.

The changes which appear to take place in the lunar formations owing to

the change in their illumination are much more striking and varied than

would be anticipated. But the question arises whether all the changes that

are associated with the progress of the lunar day can be ascribed to this

effect. Thus, Prof. W. H. Pickering writes concerning a well-known pair of

little craters of about nine miles in diameter, "known as Messier and

Messier A, situated side by side not far from the centre of the Mare

Fecunditatis. When the Sun rises first on them, the eastern one, A, is

triangular and larger than Messier, which latter is somewhat pear-shaped.

About three days after sunrise they both suddenly turn white, Messier

rapidly grows in size, soon surpasses A, and also becomes triangular in

shape. Six days after sunrise the craters are again nearly of the same

size, owing to the diminution of Messier. The shape of A has become

irregular, and differs in different lunations. At nine days after sunrise

the craters are exactly alike in size and shape, both now being

elliptical, with their major axes lying in a nearly N. and S. direction.

Just before sunset A is again the larger, being almost twice the size of

Messier."[12]

Some observers explain this cycle of changes as due merely to the peculiar

contour of the two objects, the change in the lighting during the lunar

day altering their apparent figures. Prof. W. H. Pickering, on the other

hand, while recognizing that some portion of the change of shape is

probably due to the contour of the ground, conceives that, in order to

explain the whole phenomenon, it is necessary to suppose that a white

layer of hoar frost is formed periodically round the two craters. It is

also alleged that whereas Maedler described the two craters as being

exactly alike eighty years ago, Messier A is now distinctly the larger;

but it is very doubtful whether Maedler's description can be trusted to

this degree of nicety. If it could, this would establish a permanent

change in the actual structure of the lunar surface at this point.

There are several other cases of the same order of ambiguity. The most

celebrated is Linne, a white spot about six miles in diameter on the Mare

Serentatis. This object appears to change in size during the progress of

the lunar day, and, as with Messier, some selenographers consider that it

has also suffered an actual permanent change in shape within the last

sixty or seventy years. Here again the evidence is not decisive; Neison is

by no means convinced that a change has taken place, yet does not think it

impossible that Linne may once have been a crater with steep walls which

have collapsed into its interior through the force of gravity.

Another type of suspected change is associated with the neighbourhood of

Aristarchus, the brightest formation on the Moon, so bright indeed that

Sir William Herschel, observing it when illuminated by earthshine in the

dark portion of the Moon, thought that he was watching a lunar volcano in

eruption. In 1897, on September 21, the late Major Molesworth noticed that

the crater was at that time under the rays of the setting Sun, and filled

with shadow, and the inner terraces, which should have been invisible,

were seen as faint, knotted, glimmering streaks under both the eastern and

western walls, and the central peak was also dimly discernible. He thought

this unusual lighting up of rocks on which the Sun had already set might

be due either to phosphorescence produced by long exposure to the Sun's

rays, or to inherent heat, or to reflected glare from the western rampart.

Still more important, both Major Molesworth and Mr. Walter Goodacre, each

on more than one occasion, observed what seemed to be a faint bluish mist

on the inner slope of the east wall, soon after sunrise, but this was

visible only for a short time. Other selenographers too, on rare

occasions, have made observations accordant with these, relating to

various regions on the Moon.

These, and a few other similar instances, are all that selenography has to

offer by way of evidence of actual lunar change. Of seeming change there

is abundance, but beyond that we have only cases for controversy, and one

of the most industrious of the present-day observers of the Moon, M.

Philip Fauth, declares that "as a student of the Moon for the last twenty

years, and as probably one of the few living investigators who have kept

in practical touch with the results of selenography, he is bound to

express his conviction that no eye has ever seen a physical change in the

plastic features of the Moon's surface."[13]

In this matter of change, then, the Earth and Moon stand in the greatest

contrast to each other. As we have seen, from the view-point of the Moon,

the appearance of the Earth would change so manifestly with the progress

of the seasons that no one could fail to remark the difference, even

though observing with the naked eye. But from the view-point of the Earth,

the Moon when examined by our most experienced observers, armed with our

most powerful telescopes, offers us only a few doubtful enigmatical

instances of possible change confined to small isolated localities; we see

no evidence that the "gloom of iron substance" below is ever concealed by

a veil of changing vegetation, or that "between the burning light and deep

vacuity" of the heavens above, the veil of the flying vapour has ever been

spread out. We see the Moon so clearly that we are assured it holds no

water to nourish plant life; we see it so clearly because there is no air

to carry the vapour that might dim our view.

Life is change, and a planet where there is no change, or where that

change is very small, can be no home for life. The "stability and

insensibility" are indeed required in the platform upon which life is to

appear, but there must be the presence of "the passion and the perishing,"

or life will be unable to find a home.

We infer the absence of water and air from the Moon not only from the

unchanging character of its features and the distinctness with which we

see them; we are able to make direct observations. Galileo, the first man

to observe the Moon to better advantage than with the naked eye, was not

long before he decided that the Moon contained no water, for though

Milton, in a well-known passage, makes Galileo discover

"Rivers or mountains on her spotty globe,"

Galileo himself wrote: "I do not believe that the body of the Moon is

composed of earth and water." The name of _maria_ was given to the great

grey plains of the Moon by Hevelius, but this was simply for convenience

of nomenclature, not because he actually believed them to be seas. One

observation is, in itself, sufficient to prove that the maria are not

water surfaces. The Moon's "terminator," that is to say, the line dividing

the part in sunlight from that in darkness, is clearly irregular when it

passes over the great plains; were they actually sea it would be a bright

line and perfectly smooth. The grey plains are therefore not expanses of

water now, nor were they in time past. It is obvious that in some remote

antiquity their surface was in a fluid condition, but it was the fluidity

of molten rock. This is seen by the way in which the maria have invaded,

breached, broken down, and submerged many of the circular formations on

their margins. Thus the Mare Humorum has swept away half the wall of the

rings, Hippalus and Doppelmayer, and far out in the open plain of the Mare

Nubium, great circles like Kies, and that immediately north of Flamsteed,

stand up in faint relief as of half-submerged rings. Clearly there was a

period after the age in which the great ring mountains and walled plains

came into existence, when an invasive flood attacked and partially

destroyed a large proportion of them. And the flood itself evidently

became more viscous and less fluid the further it spread from its original

centre of action, for the ridges and crumpling of the surface indicate

that the material found more and more difficulty in its flow.

We have evidence just as direct that there is no atmosphere. This is very

strikingly shown when the Moon, in its monthly progress among the stars,

passes before one of them and occults it. Such an occultation is

instantaneous, and is particularly impressive when either a disappearance

or a reappearance occurs at the defective limb; that is to say, at the

limb which is not illuminated by the Sun, and is therefore invisible. The

observer may have a bright star in the field of view, showing steadily in

a cloudless sky; there is not a hint of a weakening in its light; suddenly

it is gone. The first experience of such an observation is most

disconcerting; it is hardly less disconcerting to observe the reappearance

at the dark limb. One moment the field of view of the telescope is empty;

the next, without any sort of dawning, a bright star is shining steadily

in the void, and it almost seems to the observer as if an explosion had

taken place. If the Moon had an atmosphere extending upwards from its

surface in all directions and of any appreciable density, an occultation

would not be so exceedingly abrupt; and, in particular, if the occultation

were watched through a spectroscope, then, at the disappearance, the

spectrum of the star would not vanish as a whole, but the red end would go

first, and the rest of the spectrum would be swept out of sight

successively, from orange to the violet. This does not happen; the whole

spectrum goes out together, and it is clear that no appreciable atmosphere

can exist on the Moon. In actual observation so inappreciable is it that

its density at the Moon's surface is variously estimated as 1/300th of

that of the Earth by Neison, and as 1/10000th by W. H. Pickering. If the

Moon possessed an atmosphere bearing the same proportion to her total mass

as we find in the case of the Earth, she would have a density of

one-fortieth of our atmosphere at the sea level.

The Moon is at the same mean distance from the Sun as the Earth, and

therefore, surface for surface, receives from it on the average the same

amount of light and heat. But it makes a very different use of these

supplies. Bright as the Moon appears when seen at the full on some winter

night, it has really but a very low power of reflection, and is only

bright by contrast with the darkness of the midnight sky. If the full Moon

is seen in broad daylight, it is pale and ghost-like. Sir John Herschel

has put it on record that when in South Africa he often had the

opportunity of comparing the Moon with the face of Table Mountain, the Sun

shining full upon both, and the Moon appeared no brighter than the

weathered rock. The best determinations of the _albedo_ of the Moon, that

is to say, of its reflective power, give it as 0.17, so that only

one-sixth of the incident light is reflected, the other five-sixths being

absorbed. It is difficult to obtain a good determination of the Earth's

_albedo_, but the most probable estimate puts it as about 0.50, or three

times as great as that of the Moon. This high reflective power is partly

to be accounted for by the great extent of the terrestrial polar caps, but

chiefly by the clouds and dust layer always present in its atmosphere.

A larger proportion, therefore, of the solar rays are employed in heating

the soil of the Moon than in heating that of the Earth, and in this

connection the effect of an important difference between the two worlds

must be noted. The Earth rotates on its axis in 23 hours 56 minutes 4

seconds, the mean length of its rotation as referred to the Sun being 24

hours. The rotation of the Moon, on the other hand, takes 27 days 7 hours

43 minutes to accomplish, giving a mean rotation, as referred to the Sun,

of 29 days 12 hours 44 minutes. The lunar surface is therefore exposed

uninterruptedly to the solar scorching for very nearly fifteen of our days

at a time, and it is, in turn, exposed to the intense cold of outer space

for an equal period. As the surface absorbs heat so readily, it must

radiate it as quickly; hence radiation must go on with great rapidity

during the long lunar night. Lord Rosse and Prof. Very have both obtained

measures of the change in the lunar heat radiation during the progress of

a total eclipse of the Moon, with the result that the heat disappeared

almost completely, though not quite at the same time as the light. Prof.

Langley succeeded in obtaining from the Moon, far down in the long wave

lengths of the infra-red, a heat spectrum which was only partly due to

reflection from the Sun; part coming from the lunar soil itself, which,

having absorbed heat from the Sun, radiated it out again almost

immediately. In 1898, Prof. Very, following up Langley's line of work,

concluded that the temperature of the lunar soil must range through about

350 deg. Centigrade, considerably exceeding 100 deg. at the height of the lunar

day, and falling to about the temperature of liquid air during the lunar

night. So wide a range of temperature must be fatal to living organisms,

particularly when the range is repeated at short, regular intervals of

time. But this range of temperature comes directly from the length of the

Moon's rotation period; for the longer the day of the Moon, the higher the

temperature which may be attained in it; the longer the night, the greater

the cold which will in turn be experienced. We learn, therefore, that the

time of rotation of a planet is an important factor in its habitability.

Are the Planets Inhabited? · 第 5 / 12 章