226. _Distance of Venus from the Earth._--The distance of Venus from the

earth varies within much wider limits than that of Mercury. When Venus

is at inferior conjunction, her distance from the earth is ninety-two

million miles _minus_ sixty-seven million miles, or twenty-five million

miles; and when at superior conjunction it is ninety-two million miles

_plus_ sixty-seven million miles, or a hundred and fifty-nine million

miles. Venus is considerably more than _six times_ as far off at

superior conjunction as at inferior conjunction.

[Illustration: Fig. 258.]

227. _Apparent Size of Venus._--Owing to the great variation in the

distance of Venus from the earth, her apparent diameter varies from

about ten seconds to about sixty-six seconds. Fig. 258 shows the

apparent size of Venus at her extreme and mean distances from the earth.

228. _Volume and Density of Venus._--The real size of Venus is about the

same as that of the earth, her diameter being only about three hundred

miles less. The comparative sizes of the two planets are shown in Fig.

259. The density of Venus is a little less than that of the earth.

[Illustration: Fig. 259.]

229. _The Greatest Elongation of Venus._--Venus, like Mercury, appears

to oscillate to and fro across the sun. The angular value of the

greatest elongation of Venus varies but slightly, its greatest value

being about forty-seven degrees.

230. _Sidereal and Synodical Periods of Venus._--The _sidereal_ period

of Venus, or that of a complete revolution around the sun, is about two

hundred and twenty-five days; her orbital motion being at the rate of

nearly twenty-two miles a second. Her _synodical_ period, or the time it

takes her to pass around from her greatest eastern elongation to the

same elongation again, is about five hundred and eighty-four days, or

eighteen months. Venus is a hundred and forty-six days, or nearly five

months, in passing from her greatest elongation east through inferior

conjunction to her greatest elongation west.

231. _Venus as a Morning and an Evening Star._--For a period of about

nine months, while Venus is passing from superior conjunction to her

greatest eastern elongation, she will be east of the sun, and will

therefore set after the sun. During this period she is the _evening

star_, the _Hesperus_ of the ancients. While passing from inferior

conjunction to superior conjunction, Venus is west of the sun, and

therefore rises before the sun. During this period of nine months she is

the _morning star_, the _Phosphorus_, or _Lucifer_, of the ancients.

232. _Brilliancy of Venus._--Next to the sun and moon, Venus is at times

the most brilliant object in the heavens, being bright enough to be seen

in daylight, and to cast a distinct shadow at night. Her brightness,

however, varies considerably, owing to her phases and to her varying

distance from the earth. She does not appear brightest when at full, for

she is then farthest from the earth, at superior conjunction; nor does

she appear brightest when nearest the earth, at inferior conjunction,

for her phase is then a thin crescent (see Fig. 258). She is most

conspicuous while passing from her greatest eastern elongation to her

greatest western elongation. After she has passed her eastern

elongation, she becomes brighter and brighter till she is within about

forty degrees of the sun. Her phase at this point in her orbit is shown

in Fig. 260. Her brilliancy then begins to wane, until she comes too

near the sun to be visible. When she re-appears on the west of the sun,

she again becomes more brilliant; and her brilliancy increases till she

is about forty degrees from the sun, when she is again at her brightest.

Venus passes from her greatest brilliancy as an evening star to her

greatest brilliancy as a morning star in about seventy-three days. She

has the same phase, and is at the same distance from the earth, in both

cases of maximum brilliancy. Of course, the brilliancy of Venus when at

the maximum varies somewhat from time to time, owing to the

eccentricities of the orbits of the earth and of Venus, which cause her

distance from the earth, at her phase of greatest brilliancy, to vary.

She is most brilliant when the phase of her greatest brilliancy occurs

when she is at her aphelion and the earth at its perihelion.

[Illustration: Fig. 260.]

233. _The Atmosphere and Surface of Venus._--Schröter believed that he

saw shadings and markings on Venus similar to those on Mercury,

indicating the presence of an atmosphere and of elevations on the

surface of the planet. Fig. 261 represents the surface of Venus as it

appeared to this astronomer. By watching certain markings on the disk of

Venus, Schröter came to the conclusion that Venus rotates on her axis in

about twenty-four hours.

[Illustration: Fig. 261.]

It is now generally conceded that Venus has a dense atmosphere; but

Schröter's observations of the spots on her disk have not been verified

by modern astronomers, and we really know nothing certainly of her

rotation.

234. _Transits of Venus._--When Venus happens to be near one of the

nodes of her orbit when she is in inferior conjunction, she makes a

transit across the sun's disk. These transits occur in pairs, separated

by an interval of over a hundred years. The two transits of each pair

are separated by an interval of eight years, the dates of the most

recent being 1874 and 1882. Venus, like Mercury, appears surrounded with

a border on passing across the sun's disk, as shown in Fig. 262.

[Illustration: Fig. 262.]

Mars.

235. _The Orbit of Mars._--The orbit of Mars is more eccentric than that

of any of the larger planets, except Mercury; its eccentricity being

about one-eleventh. The inclination of the orbit to the ecliptic is

somewhat under two degrees. The mean distance of Mars from the sun is

about a hundred and forty million miles; but, owing to the eccentricity

of his orbit, the distance varies from a hundred and fifty-three million

miles to a hundred and twenty-seven million miles.

[Illustration: Fig. 263.]

236. _Distance of Mars from the Earth._--It will be seen, from Fig. 263,

that a _superior_ planet (or one outside the orbit of the earth), like

Mars, is nearer the earth, by the whole diameter of the earth's orbit,

when in opposition than when in conjunction. The mean distance of Mars

from the earth, at the time of opposition, is a hundred and forty

million miles _minus_ ninety-two million miles, or forty-eight million

miles. Owing to the eccentricity of the orbit of the earth and of Mars,

the distance of this planet when in opposition varies considerably. When

the earth is in aphelion, and Mars in perihelion, at the time of

opposition, the distance of the planet from the earth is only about

thirty-three million miles. On the other hand, when the earth is in

perihelion, and Mars in aphelion, at the time of opposition, the

distance of the planet is over sixty-two million miles.

The mean distance of Mars from the earth when in conjunction is a

hundred and forty million miles _plus_ ninety-two million miles, or two

hundred and thirty-two million miles. It will therefore be seen that

Mars is nearly five times as far off at conjunction as at opposition.

[Illustration: Fig. 264.]

237. _The Apparent Size of Mars._--Owing to the varying distance of Mars

from the earth, the apparent size of the planet varies almost as much as

that of Venus. Fig. 264 shows the apparent size of Mars at its extreme

and mean distances from the earth. The apparent diameter varies from

about four seconds to about thirty seconds.

[Illustration: Fig. 265.]

238. _The Volume and Density of Mars._--Among the larger planets Mars is

next in size to Mercury. Its real diameter is somewhat more than four

thousand miles, and its bulk is about one-seventh of that of the earth.

Its size, compared with that of the earth, is shown in Fig. 265.

[Illustration: Plate 4.]

The density of Mars is only about three-fourths of that of the earth.

239. _Sidereal and Synodical Periods of Mars._--The _sidereal_ period of

Mars, or the time in which he makes a complete revolution around the

sun, is about six hundred and eighty-seven days, or nearly twenty-three

months; but he is about seven hundred and eighty days in passing from

opposition to opposition again, or in performing a _synodical_

revolution. Mars moves in his orbit at the rate of about fifteen miles a

second.

240. _Brilliancy of Mars._--When near his opposition, Mars is easily

recognized with the naked eye by his fiery-red light. He is much more

brilliant at some oppositions than at others, for reasons already

explained (236), but always shines brighter than an ordinary star of the

first magnitude.

241. _Telescopic Appearance of Mars._--When viewed with a good telescope

(see Plate IV.), Mars is seen to be covered with dusky, dull-red

patches, which are supposed to be continents, like those of our own

globe. Other portions, of a greenish hue, are believed to be tracts of

water. The ruddy color, which overpowers the green, and makes the whole

planet seem red to the naked eye, was believed by Sir J. Herschel to be

due to an ochrey tinge in the general soil, like that of the red

sandstone districts on the earth. In a telescope, Mars appears less red,

and the higher the power the less the intensity of the color. The disk,

when well seen, is mapped out in a way which gives at once the

impression of land and water. The bright part is red inclining to

orange, sometimes dotted with brown and greenish points. The darker

spaces, which vary greatly in depth of tone, are of a dull gray-green,

having the aspect of a fluid which absorbs the solar rays. The

proportion of land to water on the earth appears to be reversed on Mars.

On the earth every continent is an island; on Mars all seas are lakes.

Long, narrow straits are more common than on the earth; and wide

expanses of water, like our Atlantic Ocean, are rare. (See Fig. 266.)

[Illustration: Fig. 266.]

[Illustration: Fig. 267.]

Fig. 267 represents a chart of the surface of Mars, which has been

constructed from careful telescopic observation. The outlines, as seen

in the telescope, are, however, much less distinct than they are

represented here; and it is by no means certain that the light and dark

portions are bodies of land and water.

In the vicinity of the poles brilliant white spots may be noticed, which

are considered by many astronomers to be masses of snow. This conjecture

is favored by the fact that they appear to diminish under the sun's

influence at the beginning of the Martial summer, and to increase again

on the approach of winter.

242. _Rotation of Mars._--On watching Mars with a telescope, the spots

on the disk are found to move (as shown in Fig. 268) in a manner which

indicates that the planet rotates in about twenty-four hours on an axis

inclined about twenty-eight degrees from a perpendicular to the plane of

its orbit. The inclination of the axis is shown in Fig. 269. It is

evident from the figure that the variation in the length of day and

night, and the change of seasons, are about the same on Mars as on the

earth. The changes will, of course, be somewhat greater, and the seasons

will be about twice as long.

[Illustration: Fig. 268.]

[Illustration: Fig. 269.]

[Illustration: Fig. 270.]

243. _The Satellites of Mars._--In 1877 Professor Hall of the Washington

Observatory discovered that Mars is accompanied by two small moons,

whose orbits are shown in Fig. 270. The inner satellite has been named

_Phobos_, and the outer one _Deimos_. It is estimated that the diameter

of the outer moon is from five to ten miles, and that of the inner one

from ten to forty miles.

Phobos is remarkable for its nearness to the planet and the rapidity of

its revolution, which is performed in seven hours thirty-eight minutes.

Its distance from the centre of the planet is about six thousand miles,

and from the surface less than four thousand. Astronomers on Mars, with

telescopes and eyes like ours, could readily find out whether this

satellite is inhabited, the distance being less than one-sixtieth of

that of our moon.

It will be seen that Phobos makes about three revolutions to one

rotation of the planet. It will, of course, rise in the west; though the

sun, the stars, and the other satellite rise in the east. Deimos makes a

complete revolution in about thirty hours.

III. THE ASTEROIDS.

244. _Bode's Law of Planetary Distances._--There is a very remarkable

law connecting the distances of the planets from the sun, which is

generally known by the name of _Bode's Law_. Attention was drawn to it

in 1778 by the astronomer Bode, but he was not really its author.

To express this law we write the following series of numbers:--

0, 3, 6, 12, 24, 48, 96;

each number, with the exception of the first, being double the one which

precedes it. If we add 4 to each of these numbers, the series becomes--

4, 7, 10, 16, 28, 52, 100;

which series was known to Kepler. These numbers, with the exception of

28, are sensibly proportional to the distances of the principal planets

from the sun, the actual distances being as follows:--

Mercury. Venus. Earth. Mars. ---- Jupiter. Saturn.

3·9 7·2 10 15·2 52·9 95·4

245. _The First Discovery of the Asteroids._--The great gap between Mars

and Jupiter led astronomers, from the time of Kepler, to suspect the

existence of an unknown planet in this region; but no such planet was

discovered till the beginning of the present century. _Ceres_ was

discovered Jan. 1, 1801, _Pallas_ in 1802, _Juno_ in 1804, and _Vesta_

in 1807. Then followed a long interval of thirty-eight years before

_Astræa_, the fifth of these minor planets, was discovered in 1845.

246. _Olbers's Hypothesis._--After the discovery of Pallas, Olbers

suggested his celebrated hypothesis, that the two bodies might be

fragments of a single planet which had been shattered by some explosion.

If such were the case, the orbits of all the fragments would at first

intersect each other at the point where the explosion occurred. He

therefore thought it likely that other fragments would be found,

especially if a search were kept up near the intersection of the orbits

of Ceres and Pallas.

Professor Newcomb makes the following observations concerning this

hypothesis:--

"The question whether these bodies could ever have formed a single

one has now become one of cosmogony rather than of astronomy. If a

planet were shattered, the orbit of each fragment would at first

pass through the point at which the explosion occurred, however

widely they might be separated through the rest of their course;

but, owing to the secular changes produced by the attractions of the

other planets, this coincidence would not continue. The orbits would

slowly move away, and after the lapse of a few thousand years no

trace of a common intersection would be seen. It is therefore

curious that Olbers and his contemporaries should have expected to

find such a region of intersection, as it implied that the explosion

had occurred within a few thousand years. The fact that the required

conditions were not fulfilled was no argument against the

hypothesis, because the explosion might have occurred millions of

years ago; and in the mean time the perihelion and node of each

orbit would have made many entire revolutions, so that the orbits

would have been completely mixed up.... A different explanation of

the group is given by the nebular hypothesis; so that Olbers's

hypothesis is no longer considered by astronomers."

247. _Later Discoveries of Asteroids._--Since 1845 over two hundred

asteroids have been discovered. All these are so small, that it requires

a very good telescope to see them; and even in very powerful telescopes

they appear as mere points of light, which can be distinguished from the

stars only by their motions.

To facilitate the discovery of these bodies, very accurate maps have

been constructed, including all the stars down to the thirteenth

magnitude in the neighborhood of the ecliptic. A reduced copy of one of

these maps is shown in Fig. 271.

[Illustration: Fig. 271.]

Furnished with a map of this kind, and with a telescope powerful enough

to show all the stars marked on it, the observer who is searching for

these small planets will place in the field of view of his telescope six

spider-lines at right angles to each other, and at equal distances

apart, in such a manner that several small squares will be formed,

embracing just as much of the heavens as do those shown in the map. He

will then direct his telescope to the region of the sky he wishes to

examine, represented by the map, so as to be able to compare

successively each square with the corresponding portion of the sky. Fig.

272 shows at the right hand the squares in the telescopic field of view,

and at the left hand the corresponding squares of the map.

[Illustration: Fig. 272.]

He can then assure himself if the numbers and positions of the stars

mapped, and of the stars observed, are identical. If he observes in the

field of view a luminous point which is not marked in the map, it is

evident that either the new body is a star of variable brightness which

was not visible at the time the map was made, or it is a planet, or

perhaps a comet. If the new body remains fixed at the same point, it is

the former; but, if it changes its position with regard to the

neighboring stars, it is the latter. The motion is generally so

sensible, that in the course of one evening the change of position may

be detected; and it can soon be determined, by the direction and rate of

the motion, whether the body is a planet or a comet.

IV. OUTER GROUP OF PLANETS.

Jupiter.

248. _Orbit of Jupiter._--The orbit of Jupiter is inclined only a little

over one degree to the ecliptic; and its eccentricity is only about half

of that of Mars, being less than one-twentieth. The mean distance of

Jupiter from the sun is about four hundred and eighty million miles;

but, owing to the eccentricity of his orbit, his actual distance from

the sun ranges from four hundred and fifty-seven to five hundred and

three million miles.

249. _Distance of Jupiter from the Earth._--When Jupiter is in

opposition, his mean distance from the earth is four hundred and eighty

million miles _minus_ ninety-two million miles, or three hundred and

eighty-eight million miles, and, when he is in conjunction, four hundred

and eighty million miles _plus_ ninety-two million miles, or five

hundred and seventy-two million miles. It will be seen that he is less

than twice as far off in conjunction as in opposition, and that the

ratio of his greatest to his least distance is very much less than in

the case of Venus and Mars. This is owing to his very much greater

distance from the sun. Owing to the eccentricities of the orbits of the

earth and of Jupiter, the greatest and least distances of Jupiter from

the earth vary somewhat from year to year.

[Illustration: Fig. 273.]

250. _The Brightness and Apparent Size of Jupiter._--The apparent

diameter of Jupiter varies from about fifty seconds to about thirty

seconds. His apparent size at his extreme and mean distances from the

earth is shown in Fig. 273.

Jupiter shines with a brilliant white light, which exceeds that of every

other planet except Venus. The planet is, of course, brightest when near

opposition.

251. _The Volume and Density of Jupiter._--Jupiter is the "giant planet"

of our system, his mass largely exceeding that of all the other planets

combined. His mean diameter is about eighty-five thousand miles; but the

equatorial exceeds the polar diameter by five thousand miles. In volume

he exceeds our earth about thirteen hundred times, but in mass only

about two hundred and thirteen times. His specific gravity is,

therefore, far less than that of the earth, and even less than that of

water. The comparative size of Jupiter and the earth is shown in Fig.

274.

[Illustration: Fig. 274.]

252. _The Sidereal and Synodical Periods of Jupiter._--It takes Jupiter

nearly twelve years to make a _sidereal_ revolution, or a complete

revolution around the sun, his orbital motion being at the rate of about

eight miles a second. His _synodical_ period, or the time of his passage

from opposition to opposition again, is three hundred and ninety-eight

days.

253. _The Telescopic Aspect of Jupiter._--There are no really permanent

markings on the disk of Jupiter; but his surface presents a very

diversified appearance. The earlier telescopic observers descried dark

belts across it, one north of the equator, and the other south of it.

With the increase of telescopic power, it was seen that these bands were

of a more complex structure than had been supposed, and consisted of

stratified, cloud-like appearances, varying greatly in form and number.

These change so rapidly, that the face of the planet rarely presents the

same appearance on two successive nights. They are most strongly marked

at some distance on each side of the planet's equator, and thus appear

as two belts under a low magnifying power.

Both the outlines of the belts, and the color of portions of the planet,

are subject to considerable changes. The equatorial regions, and the

spaces between the belts generally, are often of a rosy tinge. This

color is sometimes strongly marked, while at other times hardly a trace

of it can be seen. A general telescopic view of Jupiter is given in

Plate V.

[Illustration: Plate 5.]

254. _The Physical Constitution of Jupiter._--From the changeability of

the belts, and of nearly all the visible features of Jupiter, it is

clear that what we see on that planet is not the solid nucleus, but

cloud-like formations, which cover the entire surface to a great depth.

The planet appears to be covered with a deep and dense atmosphere,

filled with thick masses of clouds and vapor. Until recently this

cloud-laden atmosphere was supposed to be somewhat like that of our

globe; but at present the physical constitution of Jupiter is believed

to resemble that of the sun rather than that of the earth. Like the sun,

he is brighter in the centre than near the edges, as is shown in the

transits of the satellites over his disk. When the satellite first

enters on the disk, it commonly seems like a bright spot on a dark

background; but, as it approaches the centre, it appears like a dark

spot on the bright surface of the planet. The centre is probably two or

three times brighter than the edges. This may be, as in the case of the

sun, because the light near the edge passes through a greater depth of

atmosphere, and is diminished by absorption.

It has also been suspected that Jupiter shines partly by his own light,

and not wholly by reflected sunlight. The planet cannot, however, emit

any great amount of light; for, if it did, the satellites would shine by

this light when they are in the shadow of the planet, whereas they

totally disappear. It is possible that the brighter portions of the

surface are from time to time slightly self-luminous.

[Illustration: Fig. 275.]

Again: the interior of Jupiter seems to be the seat of an activity so

enormous that it can be ascribed only to intense heat. Rapid movements

are always occurring on his surface, often changing its aspect in a few

hours. It is therefore probable that Jupiter is not yet covered by a

solid crust, and that the fiery interior, whether liquid or gaseous, is

surrounded by the dense vapors which cease to be luminous on rising into

the higher and cooler regions of the atmosphere. Figs. 275 and 276 show

the disk of Jupiter as it appeared in December, 1881.

[Illustration: Fig. 276.]

255. _Rotation of Jupiter_.--Spots are sometimes visible which are much

more permanent than the ordinary markings on the belts. The most

remarkable of these is "the great red spot," which was first observed in

July, 1878, and is still to be seen in February, 1882. It is shown just

above the centre of the disk in Fig. 275. By watching these spots from

day to day, the time of Jupiter's axial rotation has been found to be

about nine hours and fifty minutes.

The axis of Jupiter deviates but slightly from a perpendicular to the

plane of its orbit, as is shown in Fig. 277.

[Illustration: Fig. 277.]

THE SATELLITES OF JUPITER.

[Illustration: Fig. 278.]

The Heavens Above: A Popular Handbook of Astronomy · 第 12 / 19 段