Among the Maria which exhibit the most remarkable arrangement of

ridges is the Mare Humorum, in the southeastern quadrant. Here, if

it be observed under a rising sun, a number of these objects will be

seen extending from the region north of the ring-mountain Vitello in

long undulating lines, roughly concentric with the western border

of the “sea,” and gradually diminishing in altitude as they spread

out, with many ramifications, to a distance of 200 miles or more

toward the north. At this stage of illumination they are strikingly

beautiful in a good telescope, reminding one of the ripple-marks left

by the tide on a soft, sandy beach. Like most other objects of their

class, they are very evanescent, gradually disappearing as the sun

rises higher in the lunar firmament, and ultimately leaving nothing

to indicate their presence beyond here and there a ghostly streak or

vein of a somewhat lighter hue than that of the neighboring surface.

The Maria, like almost every other part of the visible surface,

abound in craters of a minute type, which are scattered here

and there without any apparent law or ascertained principle of

arrangement.

Walled-plains, approximating more or less to the circular form,

though frequently deviating considerably from it, are among the

largest inclosures on the moon. They vary from upward of 150 to 160

miles or under in diameter, and are often encircled by a complex

rampart of considerable breadth, rising in some instances to a height

of 12,000 feet or more above the inclosed plain. This rampart is

rarely continuous, but is generally interrupted by gaps, crossed by

transverse valleys and passes and broken by more recent craters and

depressions. As a rule, the area within the circumvallation (usually

termed “the floor”) is only slightly, if at all, lower than the

region outside: it is very generally of a dusky hue, similar to that

of the gray plains of Maria, and, like them, is usually variegated

by the presence of hills, ridges, and craters, and is sometimes

traversed by delicate furrows, termed clefts or rills.

Ptolemæus, in the third quadrant and not far removed from the

centre of the disk, may be taken as a typical example of the class.

Here we have a vast plain, 115 miles from side to side, encircled

by a massive but much broken wall, which at one peak towers more

than 9,000 feet above a level floor, which includes details of a

very remarkable character. The adjoining Alphonsus is another, but

somewhat smaller object of the same type, as are also Albategnius and

Arzachel; and Plato, in a high northern latitude, with its noble,

many-peaked rampart and its variable steel-gray interior, Grimaldi,

near the eastern limb (perhaps the darkest area on the moon),

Schickard, nearly as big on the southeastern limb, and Bailly, larger

than either (still further south in the same quadrant), although they

approach some of the smaller “seas” in size, are placed in the same

category. The conspicuous central mountain, so frequently associated

with other types of ringed inclosures, is by no means invariably

found within the walled-plains; though, as in the case of Petavius,

Langrenus, Gassendi, and several other noteworthy examples, it is

very prominently displayed. The progress of sunrise on all these

objects affords a magnificent spectacle. Very often when the rays

infringe on their apparently level floor at an angle of from 1° to

2°, it is seen to be coarse, rough grained, and covered with minute

elevations, although an hour or so afterward it appears as smooth as

glass.

The more massive and extended mountain ranges of the moon are found

in the Northern Hemisphere, and (what is significant) in that

portion of it which exhibits few indications of other superficial

disturbances. The most prominently developed systems, the Alps, the

Caucasus, and the Apennines, forming a mighty western rampart to the

Mare Imbrium and giving it all the appearance of a vast walled-plain,

present few points of resemblance to any terrestrial chain. The

former include many hundred peaks, among which Mont Blanc rises to a

height of 12,000 feet, and a second, some distance west of Plato, to

nearly as great an altitude; while others ranging from 5,000 to 8,000

feet are common. They extend in a southwest direction from Plato to

the Caucasus, terminating somewhat abruptly, a little west of the

central meridian in about N. lat. 42°. One of the most interesting

features associated with this range is the so-called great Alpine

valley, which cuts through it west of Plato.

The Caucasus consist of a massive wedge-shaped mountain land,

projecting southward, and partially dividing the Mare Imbrium from

the Mare Serenitatis, both of which they flank. Though without peaks

so lofty as those pertaining to the Alps, there is one, immediately

east of the ring-plain Calippus, which, towering to 19,000 feet,

surpasses any of which the latter system can boast. The Apennines,

however, are by far the most magnificent range on the visible

surface, including as they do some 3,000 peaks, and extending in an

almost continuous curve of more than 400 miles in length from Mount

Hadley, on the north, to the fine ring-plain Eratosthenes, which

forms a fitting termination, on the south. The great headland Mount

Hadley rises more than 15,000 feet, while a neighboring promontory on

the southeast of it is fully 14,000 feet, and another, close by, is

still higher above the Mare. Mount Huyghens, again in N. lat. 20°,

and the square-shaped mass Mount Wolf, near the southern end of the

chain, include peaks standing 18,000 and 12,000 feet respectively

above the plain to which their flanks descend with a steep declivity.

The counterscarp of the Apennines, in places 160 miles in width from

east to west, runs down to the Mare Vaporum, with a comparatively

gentle inclination. It is everywhere traversed by winding valleys

of a very intricate type, all trending toward the southwest, and

includes some very bright craters and mountain-rings.

Whether variations in the visibility of lunar details, when observed

under apparently similar conditions, actually occur from time to

time from some unknown cause, is one of those vexed questions which

will only be determined when the moon is systematically studied by

experienced observers using the finest instruments at exceptionally

good stations; but no one who examines existing records of rills by

Gruithuisen, Lohrmann, Mädler, Schmidt, and other observers, can well

avoid the conclusion that the anomalies brought to light therein

point strongly to the probability of the existence of some agency

which occasionally modifies their appearance or entirely conceals

them from view. In short, the more direct telescopic observations

accumulate, and the more the study of minute detail is extended, the

stronger becomes the conviction that, in spite of the absence of an

appreciable atmosphere, there may be something resembling low-lying

exhalations from some parts of the surface which from time to time

are sufficiently dense to obscure, or even obliterate, the region

beneath them.

Sir John Herschel maintained that “the actual illumination of the

lunar surface is not much superior to that of weathered sandstone

rock in full sunshine. I have,” he says, “frequently compared the

moon setting behind the gray perpendicular façade of the Table

Mountain, illumined by the sun just risen in the opposite quarter of

the horizon when it has been scarcely distinguishable in brightness

from the rock in contact with it. The sun and moon being at nearly

equal altitudes, and the atmosphere perfectly free from cloud or

vapor, its effect is alike on both luminaries.” Zöllner’s elaborate

researches on this question are closely in accord with the above

observational result. Though he considers that the brightest parts

of the surface are as white as the whitest objects with which we are

acquainted, yet, taking the reflected light as a whole, he finds that

the moon is more nearly black than white. The most brilliant object

on the surface is the central peak of the ring-plain Aristarchus, the

darkest the floor of Grimaldi, or perhaps a portion of that of the

neighboring Riccioli. Between these extremes there is every gradation

of tone. Proctor, discussing this question on the basis of Zöllner’s

experiments respecting the light reflected by various substances,

concludes that the dark area just mentioned must be notably darker

than the dark gray syenite which figures in his tables, while the

floor of Aristarchus is as white as newly fallen snow.

MARS.—AGNES M. CLERKE

The furthest terrestrial planet from the sun is Mars, the “star of

strength.” No other heavenly body, except the moon, is so well placed

for observation from our position in space.

The diameter of Mars is 4,200 miles; its surface is equal to

two-sevenths, its volume to one-seventh those of the earth. But, in

consequence of its inferior mean density, nine such spheres would go

to make up the mass of our world. The superficial force of gravity

on Mars, compared with its terrestrial value, is as thirty-eight to

a hundred. A man could leap there a wall eight feet four inches in

height with no more effort than it would cost him here to spring over

a two-foot fence.

The planet’s rotation is performed in 24 hours, 37 minutes, on an

axis deviating from the vertical by 24° 50′. Hence its seasons

resemble our own, except in being nearly twice as long, for the

Martian year is of 687 days.

The disk of Mars is diversified with three shades of color—reddish,

or dull orange, dark grayish-green, and pure white. The last shows

mainly in two diametrically opposite patches. Each pole is surrounded

by a brilliant cap, suggesting the deposition of ice or snow over

the chilly spaces corresponding to our arctic and antarctic regions.

Nor is this all. Each of the polar hoods shrinks to a mere remnant

as the local summer advances, but regains its original size when

wintry influences are again in the ascendant. Here, and nowhere

else in the planetary system, we meet evidence of seasonal change;

and seasonal change is associated with vital possibilities. Again,

a globe upon which snow visibly melts must contain water; hence

the green markings can not but image to our minds seas and inlets

subdividing continents, the blond complexion of which may be caused

by some native peculiarity of the soil. It is in no way connected

with vegetation, since it neither fades nor flushes with the advent

of spring; and an atmospheric origin is excluded by the circumstance

that it becomes effaced by a whitish haze near the limb, just where

the densest atmospheric strata are traversed by the line of sight.

The spots on Mars are by no means so sharply defined as lunar craters

and _maria_; yet they are fundamentally permanent. Some can be

recognized from drawings made over two hundred years ago; and these

antique records have served modern astronomers to determine with

minute accuracy the rotation-period of the planet. Continents are

somewhat vaguely outlined. Great tracts of them are of an uncertain

and variable hue, as if subject to inundations. This peculiarity,

thoroughly certified during the favorable opposition of 1892, makes

a strong distinction between Mars and the Earth. Terrestrial oceans

keep within the limits assigned to them. On the neighboring planet—as

M. Faye observed in 1892—“water seems to march about at its ease,”

flooding from time to time regions as wide as France. The imperfect

separation of the two elements recalls the conditions prevailing

during the terrestrial carboniferous era.

The main part of the land of Mars is situated in the Northern

Hemisphere. It covers two-thirds of the entire globular surface.

Rather than land, indeed, it should be called a network of land and

water. The great continental block—so its orange tint declares it to

be—is cut up in all possible directions by an intricate system of

what appear to be waterways, running in perfectly straight lines—that

is, along great circles of the globe—for distances varying from 350

to upward of 4,000 miles. They are frequently seen in duplicate,

strictly parallel companions developing thirty to three hundred miles

apart from the original formations. This mysterious phenomenon is

evanescent, or rather periodical.

The canals invariably connect two bodies of water; hence they need

no locks or hydraulic machinery; their course is on a dead level.

The broadest of them are comparable with the Adriatic; those at the

limit of visibility, stretching like the finest spider-threads across

the disk, have a width of eighteen miles. “The canals,” Schiaparelli

says, “may intersect among themselves at all possible angles, but

by preference they converge toward the small spots to which we have

given the name of lakes. For example, seven are seen to converge in

Lacus Phœnicis, eight in Trivium Charontis, six in Lunæ Lacus, and

six in Ismenius Lacus.”

These “lakes” evidently form an integral part of the canal system.

They resemble huge railway junctions; and the largest of them—the

“Eye of Mars” (Schiaparelli’s Lacus Solis)—seems, in Mr. Lowell’s

phrase, like the hub of a five-spoked wheel. Mr. W. H. Pickering

in 1892, and Mr. Percival Lowell in 1894, were amazed at their

extraordinary abundance.

“Scattered over the orange-ochre groundwork of the continental

regions of the planet,” the latter wrote, “are any number of dark,

round spots. How many there may be it is not possible to state, as

the better the seeing, the more of them there seem to be. In spite,

however, of their great number, there is no instance of one occurring

unconnected with a canal. What is more, there is apparently none

which does not lie at the junction of several canals. Reversely, all

the junctions appear to be provided with spots.”

Most of these foci are about 120 miles in diameter, and appear most

precisely circular when most clearly seen. “Plotted upon a globe,”

Mr. Lowell continues, “they and their connecting canals make a

most curious network over all the orange-ochre equatorial parts of

the planet, a mass of lines and knots, the one marking being as

omnipresent as the other. Indeed, the spots are as peculiar and

distinctive a feature of Mars as the canals themselves.”

Like the canals, too, they emerge periodically, and in the same but

a retarded succession. They “are, therefore, in the first place,

seasonal phenomena, and, in the second place, phenomena that depend

for their existence upon the prior existence of the canals.”

Mr. Lowell terms them “oases,” and does not shrink from the full

implication of the term.

The most important result of the numerous observations of Mars,

made during the oppositions of 1892 and 1894, was the recognition

of a regular course of change dependent upon the succession of

its seasons. Schiaparelli had long anticipated this result; he is

commonly in advance of his time. These changes, moreover, when

closely watched, are really self-explanatory. The alternate melting

of the northern and southern snow-caps initiates and to some extent

determines them. As summer advances in either hemisphere, the wasting

of the corresponding white calotte can be followed in every minute

particular. “The snowy regions are then seen to be successively

notched at their edges; black holes and huge fissures are formed

in their interiors; great isolated fragments many miles in extent

stand out from the principal mass, dissolve, and disappear a little

later. In short, the same divisions and movements of these icy fields

present themselves to us at a glance that occur during the summer of

our own arctic regions.”

Indeed, glaciation on Mars is much less durable than on the earth. In

1894 the southern snow-cap vanished to the last speck 59 days after

the solstice and the remnant usually left looks scarcely enough to

make a comfortable cap for Ben Nevis. An immense quantity of water

is thus set free. The polar seas overflow; gigantic inundations

reinforced, doubtless, from other sources, spread to the tropics;

Syrtis regions of marsh or bog deepen in hue, and become distinctly

aqueous; canals dawn on the sight, and grow into undeniable

realities. We seem driven to believe that they discharge the function

of flood-emissaries.

Mr. Lowell does not hesitate to pronounce them of artificial

formation, and, on that large assumption, the purpose of their

connection with his “oases” becomes transparently clear. They bring

to these Tadmors in the wilderness the water supply by which they

are made to “blossom as the rose.” The junction-spots, we are told,

do not enlarge when the vernal freshet reaches them; they only

darken through the sudden development of vegetation. These circular

“districts, artificially fertilized by the canal system,” are strewn

broadcast over vast desert areas, the orange-ochreous sections of

Mars, covering the greater part of its surface, but deep buried in

the millennial dust of disintegrated red sandstone strata.

“Here, then,” Mr. Lowell remarks, “we have an end and reason for the

existence of canals, and the most natural conceivable—namely, that

the canals are constructed for the express purpose of fertilizing the

oases. When we consider the amazing system of the canal lines, we are

carried to this conclusion as forthright as is the water itself; what

we see being not the canal itself, indeed, but the vegetation along

its banks.”

The proportion of water to land is much smaller on Mars than on

the earth. Only two-sevenths of the disk are covered by the dusky

areas, and of late the aqueous nature of some, if not all, of

these has been seriously called in question. Professor Pickering

was convinced by his observations, in 1892 and 1894, “that the

permanent water area upon Mars, if it exist at all, is extremely

limited in its dimensions.” He estimated it at about half the size

of the Mediterranean. Professor Schaeberle is similarly incredulous.

If the dark markings are seas, he asks, how explain the irregular

gradations of shade in them? How, above all, explain their apparent

intersection by well-marked canals? Professor Barnard, observing

with the Lick thirty-six inch in 1894, discerned on the Martian

surface an astonishing wealth of detail, “so intricate, small, and

abundant, that it baffled all attempts to properly delineate it.”

It was embarrassing to find these minute features belonging more

characteristically to the “seas” than to the “continents.” Under the

best conditions, the dark regions lost all trace of uniformity.

Their appearance resembled that of a mountainous country, broken by

cañon, rift, and ridge, seen from a great elevation. These effects

were especially marked in the “ocean” area of the Hour-Glass Sea.

Evidently the relations of solid and liquid in that remote orb

are abnormal; they can not be completely explained by terrestrial

analogies. Yet a series of well-attested phenomena are intelligible

only on the supposition that Mars is, in some real sense, a

terraqueous globe. Where snows melt there must be water; and the

origin of the Rhone from a great glacier is scarcely more evident to

our senses than the dissolution of Martian ice-caps into pools and

streams.

The testimony of the spectroscope is to the same effect. Dr. Huggins

found, in 1867, the spectrum of Mars impressed with the distinct

traces of aqueous absorption, and the fact, although called in

question by Professor Campbell of Lick, in 1894, has been reaffirmed

both at Tulse Hill and at Potsdam. That clouds form and mists rise

in the thin Martian air, admits of doubt. During the latter half

of October, 1894, an area much larger than Europe remained densely

obscured. Whether or no actual rain was at that time falling over

the Maraldi Sea and the adjacent continent it would be useless to

conjecture. We only know that with the low barometric pressure at the

surface of Mars, the boiling point of water must be proportionately

depressed (Flammarion puts it at 115° Fahrenheit), which implies that

it evaporates rapidly, and can be transported easily.

If the Martian atmosphere be of the same proportionate mass as that

of our earth, it can possess no more than one-seventh its superficial

density. That is to say, it is more than twice as tenuous as the

air at the summits of the Himalayas. The corresponding height of

a terrestrial barometer would be four and a half inches. Owing,

however, to the reduced strength of gravity on Mars, this slender

envelope is exceedingly extensive. In the pure sky scarcely veiled by

it, the sun, diminished to less than half his size at our horizons,

probably exhibits his coronal streamers and prominences as a regular

part of his noontide glory; atmospheric circulation proceeds so

tranquilly as not to trouble the repose of a land “in which it

seemeth always afternoon”; no cyclones traverse its surface, only

mild trade-winds flow toward the equator, to supply for the volumes

of air gently lifted by the power of the sun, to carry reinforcements

of water-vapor north and south. Aerial movements are, in fact, by a

very strong presumption, of the terrestrial type, but executed with

greatly abated vigor.

Brilliant projections above the terminator of Mars were first

distinctly perceived at the Lick Observatory in 1890. They have

been reobserved at Nice, Arequipa, and Flagstaff (Mr. Lowell’s

observatory), coming into view, as a rule, when circumstances concur

to favor their visibility. They strictly resemble lunar peaks and

craters, catching the first rays of the sun, while the ground about

them is still immersed in darkness; and Professor Campbell connects

them with “mountain chains lying _across_ the terminator of the

planet,” and in some cases possibly snow-covered. He calculates their

height at about ten thousand feet. Their presence was unlooked for,

since a flat expanse is a condition _sine quâ non_ for the minute

intersection of land by water, which seems to prevail on Mars.

Although the sun is less than half as powerful on Mars as it is here,

the Martian climate, to outward appearance, compares favorably with

our own. Polar glaciation is less extensive and more evanescent, and

little snow falls outside the arctic and antarctic regions. Yet the

theoretical mean temperature is minus 4° C., or 61° of Fahrenheit

below freezing. This means a tremendous ice-grip. The coldest spot on

the earth’s surface is considerably warmer than this cruel average.

Fortunately, it exists only on paper. Some compensatory store of

warmth must then be possessed by Mars, and it can scarcely be

provided by its attenuated air. Possibly, internal heat may still be

effective, and we see exemplified in Mars the geological period when

vines and magnolias flourished in Greenland, and date-palms ripened

their fruit on the coast of Hampshire.

The climate of Mars, according to Schiaparelli, “must resemble that

of a clear day upon a high mountain. By day a very strong solar

radiation hardly at all mitigated by mist or vapor; by night a

copious radiation from the soil toward celestial space, and hence a

very marked refrigeration; consequently, a climate of extremes, and

great changes of temperature from day to night, and from one season

to another. And as on the earth, at altitudes of from 17,000 to

20,000 feet, the vapor of the atmosphere is condensed only into the

solid form, producing those whitish masses of suspended crystals

which we call cirrus-clouds, so in the atmosphere of Mars it would

be rarely possible to find collections of cloud capable of producing

rain of any consequence. The variation of temperature from one season

to another would be notably increased by their long duration, and

thus we can understand the great freezing and melting of the snow,

renewed in turn at the poles at each complete revolution of the

planet round the sun.”

The story of the universe. Volume 1 (of 4) · 第 24 / 27 段