CELESTIAL MEASUREMENTS.

"Who hath measured the waters in the hollow of his hand, and meted

out heaven with the span? Mine hand also hath laid the foundation

of the earth, and my right hand hath spanned the heavens."--_Isa._

xl. 12; xlviii. 13.

[Page 56]

"Go to yon tower, where busy science plies

Her vast antennæ, feeling thro' the skies;

That little vernier, on whose slender lines

The midnight taper trembles as it shines,

A silent index, tracks the planets' march

In all their wanderings thro' the ethereal arch,

Tells through the mist where dazzled Mercury burns,

And marks the spot where Uranus returns.

"So, till by wrong or negligence effaced,

The living index which thy Maker traced

Repeats the line each starry virtue draws

Through the wide circuit of creation's laws;

Still tracks unchanged the everlasting ray

Where the dark shadows of temptation stray;

But, once defaced, forgets the orbs of light,

And leaves thee wandering o'er the expanse of night."

OLIVER WENDELL HOLMES.

[Page 57]

IV.

_CELESTIAL MEASUREMENTS._

We know that astronomy has what are called practical uses. If a

ship had been driven by Euroclydon ten times fourteen days and

nights without sun or star appearing, a moment's glance into the

heavens from the heaving deck, by a very slightly educated sailor,

would tell within one hundred yards where he was, and determine

the distance and way to the nearest port. We know that, in all

final and exact surveying, positions must be fixed by the stars.

Earth's landmarks are uncertain and easily removed; those which

we get from the heavens are stable and exact.

In 1878 the United States steam-ship _Enterprise_ was sent to survey

the Amazon. Every night a "star party" went ashore to fix the exact

latitude and longitude by observations of the stars. Our real landmarks

are not the pillars we rear, but the stars millions of miles away.

All our standards of time are taken from the stars; every railway

train runs by their time to avoid collision; by them all factories

start and stop. Indeed, we are ruled by the stars even more than

the old astrologers imagined.

Man's finest mechanism, highest thought, and broadest exercise

of the creative faculty have been inspired by astronomy. No other

instruments approximate in delicacy those which explore the heavens;

no other [Page 58] system of thought can draw such vast and certain

conclusions from its premises. "Too low they build who build beneath

the stars;" we should lay our foundations in the skies, and then

build upward.

We have been placed on the outside of this earth, instead of the

inside, in order that we may look abroad. We are carried about,

through unappreciable distance, at the inconceivable velocity of

one thousand miles a minute, to give us different points of vision.

The earth, on its softly-spinning axle, never jars enough to unnest

a bird or wake a child; hence the foundations of our observatories

are firm, and our measurements exact. Whoever studies astronomy,

under proper guidance and in the right spirit, grows in thought

and feeling, and becomes more appreciative of the Creator.

_Celestial Movements._

Let it not be supposed that a mastery of mathematics and a finished

education are necessary to understand the results of astronomical

research. It took at first the highest power of mind to make the

discoveries that are now laid at the feet of the lowliest. It took

sublime faith, courage, and the results of ages of experience in

navigation, to enable Columbus to discover that path to the New

World which now any little boat can follow. Ages of experience

and genius are stored up in a locomotive, but quite an unlettered

man can drive it. It is the work of genius to render difficult

matters plain, abstruse thoughts clear.

[Illustration: Fig. 19.]

A brief explanation of a few terms will make the principles of

world inspection easily understood. Imagine a perfect circle thirty

feet in diameter--that is, create [Page 59] one (Fig. 19). Draw

through it a diameter horizontally, another perpendicularly. The

angles made by the intersecting lines are each said to be ninety

degrees, marked thus °. The arc of a circle included between any two

of the lines is also 90°. Every circle, great or small, is divided

into these 360°. If the sun rose in the east and came to the zenith

at noon, it would have passed 90°. When it set in the west it would

have traversed half the circle, or 180°. In Fig. 20 the angle of the

lines measured on the graduated arc is 10°. The mountain is 10°

high, the world 10° in diameter, the comet moves 10° a day, the

stars are 10° apart. The height of the mountain, the diameter of the

world, the velocity of the comet, and the distance between the

stars, depend on the distance of each from the point of sight. Every

degree is divided into 60 minutes (marked '), and every minute into

60 seconds (marked ").

[Illustration: Fig. 20.--Illustration of Angles.]

Imagine yourself inside a perfect sphere one hundred feet in diameter,

with the interior surface above, around, and below studded with

fixed bright points like stars. The familiar constellations of

night might be blazoned there in due proportion.

If this star-sprent sphere were made to revolve once in twenty-four

hours, all the stars would successively [Page 60] pass in review.

How easily we could measure distances between stars, from a certain

fixed meridian, or the equator! How easily we could tell when any

particular star would culminate! It is as easy to take all these

measurements when our earthly observatory is steadily revolved

within the sphere of circumambient stars. Stars can be mapped as

readily as the streets of a great city. Looking down on it in the

night, one could trace the lines of lighted streets, and judge

something of its extent and regularity. But the few lamps of evening

would suggest little of the greatness of the public buildings, the

magnificent enterprise and commerce of its citizens, or the

intelligence of its scholars. Looking up to the lamps of the

celestial city, one can judge something of its extent and

regularity; but they suggest little of the magnificence of the many

mansions.

Stars are reckoned as so many degrees, minutes, and seconds from

each other, from the zenith, or from a given meridian, or from the

equator. Thus the stars called the Pointers, in the Great Bear,

are 5° apart; the nearest one is 29° from the Pole Star, which is

39° 56' 29" above the horizon at Philadelphia. In going to England

you creep up toward the north end of the earth, till the Pole Star

is 54° high. It stays near its place among the stars continually,

"Of whose true-fixed and resting quality

There is no fellow in the firmament."

_How to Measure._

Suppose a telescope, fixed to a mural circle, to revolve on an axis,

as in Fig. 21; point it horizontally at a star; [Page 61] turn it up

perpendicular to another star. Of course the two stars are 90°

apart, and the graduated scale, which is attached to the outer edge

of the circle, shows a revolution of a quarter circle, or 90°, But a

perfect accuracy of measurement must be sought; for to mistake the

breadth of a hair, seen at the distance of one hundred and

twenty-five feet, would cause an error of 3,000,000 miles at the

distance of the sun, and immensely more at the distance of the

stars. The correction of an inaccuracy of no greater magnitude than

that has reduced our estimate of the distance of our sun 3,000,000

miles.

[Illustration: Fig. 21.--Mural Circle.]

Consider the nicety of the work. Suppose the graduated scale to

be thirty feet in circumference. Divided into 360°, each would

be one inch long. Divide each degree into 60', each one is 1/60

of an inch long. It takes good eyesight to discern it. But each

minute must be [Page 62] divided into 60", and these must not only

be noted, but even tenths and hundredths of seconds must be

discerned. Of course they are not seen by the naked eye; some

mechanical contrivance must be called in to assist. A watch loses

two minutes a week, and hence is unreliable. It is taken to a

watch-maker that every single second may be quickened 1/20160 part

of itself. Now 1/20000 part of a second would be a small interval of

time to measure, but it must be under control. If the temperature of

a summer morning rises ten or twenty degrees we scarcely notice it;

but the magnetic tastimeter measures 1/5000 of a degree.

Come to earthly matters. In 1874, after nearly twenty-eight years'

work, the State of Massachusetts opened a tunnel nearly five miles

long through the Hoosac Mountains. In the early part of the work

the engineers sunk a shaft near the middle 1028 feet deep. Then the

question to be settled was where to go so as to meet the approaching

excavations from the east and west. A compass could not be relied

on under a mountain. The line must be mechanically fixed. A little

divergence at the starting-point would become so great, miles away,

that the excavations might pass each other without meeting; the

grade must also rise toward the central shaft, and fall in working

away from it; but the lines were fixed with such infinitesimal

accuracy that, when the one going west from the eastern portal and

the one going east from the shaft met in the heart of the mountain,

the western line was only one-eighth of an inch too high, and

three-sixteenths of an inch too far north. To reach this perfect

result they had to triangulate from the eastern portal to distant

[Page 63] mountain peaks, and thence down the valley to the central

shaft, and thus fix the direction of the proposed line across the

mouth of the shaft. Plumb-lines were then dropped one thousand and

twenty-eight feet, and thus the line at the bottom was fixed.

Three attempts were made--in 1867, 1870, and 1872--to fix the exact

time-distance between Greenwich and Washington. These three separate

efforts do not differ one-tenth of a second. Such demonstrable results

on earth greatly increase our confidence in similar measurements

in the skies.

[Illustration: Fig. 22.]

A scale is frequently affixed to a pocket-rule, by which we can

easily measure one-hundredth of an inch (Fig. 22). The upper and

lower line is divided into tenths of an inch. Observe the slanting

line at the right hand. It leans from the perpendicular one-tenth

of an inch, as shown by noticing where it reaches the top line. When

it reaches the second horizontal line it has left the perpendicular

one-tenth of that tenth--that is, one-hundredth. The intersection

marks 99/100 of an inch from one end, and one-hundredth from the

other.

When division-lines, on measures of great nicety, get too fine

to be read by the eye, we use the microscope. By its means we are

able to count 112,000 lines ruled on a glass plate within an inch.

The smallest object that can be seen by a keen eye makes an angle

of 40", but by putting six microscopes on the scale of the telescope

on the mural circle, we are able to reach an exactness of 0".1, or

1/3600 of an inch. This instrument is used to measure the declination

of stars, or angular [Page 64] distance north or south of the

equator. Thus a star's place in two directions is exactly fixed.

When the telescope is mounted on two pillars instead of the face of

a wall, it is called a transit instrument. This is used to determine

the time of transit of a star over the meridian, and if the transit

instrument is provided with a graduated circle it can also be used

for the same purposes as the mural circle. Man's capacity to measure

exactly is indicated in his ascertainment of the length of waves of

light. It is easy to measure the three hundred feet distance between

the crests of storm-waves in the wide Atlantic; easy to measure the

different wave-lengths of the different tones of musical sounds. So

men measure the lengths of the undulations of light. The shortest is

of the violet light, 154.84 ten-millionths of an inch. By the

horizontal pendulum Professor Root has made 1/36000000 of an inch

apparent.

The next elements of accuracy must be perfect time and perfect

notation of time. As has been said, we get our time from the stars.

Thus the infinite and heavenly dominates the finite and earthly.

Clocks are set to the invariable sidereal time. Sidereal noon is

when we have turned ourselves under the point where the sun crosses

the equator in March, called the vernal equinox. Sidereal clocks

are figured to indicate twenty-four hours in a day: they tick exact

seconds. To map stars we wish to know the exact second when they

cross the meridian, or the north and south line in the celestial

dome above us. The telescope (Fig. 21, p. 61) swings exactly north

and south. In its focus a set of fine threads of spider-lines is

placed (Fig. 23). The telescope is set just high enough, so that

by the rolling over of the earth [Page 65] the star will come into

the field just above the horizontal thread. The observer notes the

exact second and tenth of a second when the star reaches each

vertical thread in the instrument, adds together the times and

divides by five to get the average, and the exact time is reached.

[Illustration: Fig. 23.--Transit of a Star noted.]

But man is not reliable enough to observe and record with sufficient

accuracy. Some, in their excitement, anticipate its positive passage,

and some cannot get their slow mental machinery in motion till

after it has made the transit. Moreover, men fall into a habit of

estimating some numbers of tenths of a second oftener than others.

It will be found that a given observer will say three tenths or

seven tenths oftener than four or eight. He is falling into ruts,

and not trustworthy. General O. M. Mitchel, who had been director

of the Cincinnati Observatory, once told one of his staff-officers

that he was late at an appointment. "Only a few minutes," said the

officer, apologetically. "Sir," said the general, "where I have

been accustomed to work, hundredths of a second are too important

to be neglected." And it is to the rare genius of this astronomer,

and to others, that we owe the mechanical accuracy that we now

attain. The clock is made to mark its seconds on paper wrapped

around a revolving cylinder. Under the observer's fingers is an

electric key. This he can touch at the instant of the transit of

the star [Page 66] over each wire, and thus put his observation on

the same line between the seconds dotted by the clock. Of course

these distances can be measured to minute fractional parts of a

second.

But it has been found that it takes an appreciable time for every

observer to get a thing into his head and out of his finger-ends,

and it takes some observers longer than others. A dozen men, seeing

an electric spark, are liable to bring down their recording marks

in a dozen different places on the revolving paper. Hence the time

that it takes for each man to get a thing into his head and out

of his fingers is ascertained. This time is called his personal

equation, and is subtracted from all of his observations in order to

get at the true time; so willing are men to be exact about material

matters. Can it be thought that moral and spiritual matters have

no precision? Thus distances east or west from any given star or

meridian are secured; those north and south from the equator or

the zenith are as easily fixed, and thus we make such accurate

maps of the heavens that any movements in the far-off stars--so

far that it may take centuries to render the swiftest movements

appreciable--may at length be recognized and accounted for.

[Illustration: Fig. 24.]

We now come to a little study of the modes of measuring distances.

Create a perfect square (Fig. 24); draw a diagonal line. The square

angles are 90°, the divided angles give two of 45° each. Now the

base A B is equal to the perpendicular A C. Now any point--C, where

a perpendicular, A C, and a diagonal, B C, meet--will be [Page 67]

as far from A as B is. It makes no difference if a river flows

between A and C, and we cannot go over it; we can measure its

distance as easily as if we could. Set a table four feet by eight

out-doors (Fig. 25); so arrange it that, looking along one end, the

line of sight just strikes a tree the other side of the river. Go to

the other end, and, looking toward the tree, you find the line of

sight to the tree falls an inch from the end of the table on the

farther side. The lines, therefore, approach each other one inch in

every four feet, and will come together at a tree three hundred and

eighty-four feet away.

[Illustration: Fig. 25.--Measuring Distances.]

[Illustration: Fig. 26.--Measuring Elevations.]

The next process is to measure the height or magnitude of objects

at an ascertained distance. Put two pins in a stick half an inch

apart (Fig. 26). Hold it up two feet from the eye, and let the

upper pin fall in line with your eye and the top of a distant church

steeple, and the lower pin in line with the bottom of the church and

your eye. If the church is three-fourths of a mile away, it must

be eighty-two feet high; if a mile away, it must be one hundred

and ten feet high. For if two lines spread [Page 68] one-half an

inch going two feet, in going four feet they will spread an inch,

and in going a mile, or five thousand two hundred and eighty feet,

they will spread out one-fourth as many inches, viz., thirteen

hundred and twenty--that is, one hundred and ten feet. Of course

these are not exact methods of measurement, and would not be correct

to a hair at one hundred and twenty-five feet, but they perfectly

illustrate the true methods of measurement.

Imagine a base line ten inches long. At each end erect a perpendicular

line. If they are carried to infinity they will never meet: will

be forever ten inches apart. But at the distance of a foot from

the base line incline one line toward the other 63/10000000 of

an inch, and the lines will come together at a distance of three

hundred miles. That new angle differs from the former right angle

almost infinitesimally, but it may be measured. Its value is about

three-tenths of a second. If we lengthen the base line from ten

inches to all the miles we can command, of course the point of

meeting will be proportionally more distant. The angle made by

the lines where they come together will be obviously the same as

the angle of divergence from a right angle at this end. That angle

is called the parallax of any body, and is the angle that would

be made by two lines coming from that body to the two ends of any

conventional base, as the semi-diameter of the earth. That that

angle would vary according to the various distances is easily seen

by Fig. 27.

[Illustration: Fig. 27.]

Let O P be the base. This would subtend a greater angle seen from

star A than from star B. Let B be far enough away, and O P would

become invisible, and B [Page 69] would have no parallax for that

base. Thus the moon has a parallax of 57" with the semi-equatorial

diameter of the earth for a base. And the sun has a parallax 8".85

on the same base. It is not necessary to confine ourselves to right

angles in these measurements, for the same principles hold true in

any angles. Now, suppose two observers on the equator should look at

the moon at the same instant. One is on the top of Cotopaxi, on the

west coast of South America, and one on the west coast of Africa.

They are 90° apart--half the earth's diameter between them. The one

on Cotopaxi sees it exactly overhead, at an angle of 90° with the

earth's diameter. The one on the coast of Africa sees its angle with

the same line to be 89° 59' 3"--that is, its parallax is 57". Try

the same experiment on the sun farther away, as is seen in Fig. 27,

and its smaller parallax is found to be only 8".85.

It is not necessary for two observers to actually station themselves

at two distant parts of the earth in order to determine a parallax.

If an observer could go from one end of the base-line to the other,

he could determine both angles. Every observer is actually carried

along through space by two motions: one is that of the earth's

revolution of one thousand miles an hour around the axis; and the

other is the movement of the earth around the sun of one thousand

miles in a minute. Hence we can have the diameter not only of [Page

70] the earth (eight thousand miles) for a base-line, but the

diameter of the earth's orbit (184,000,000 miles), or any part of

it, for such a base. Two observers at the ends of the earth's

diameter, looking at a star at the same instant, would find that it

made the same angle at both ends; it has no parallax on so short a

base. We must seek a longer one. Observe a certain star on the 21st

of March; then let us traverse the realms of space for six months,

at one thousand miles a minute. We come round in our orbit to a

point opposite where we were six months ago, with 184,000,000 of

miles between the points. Now, with this for a base-line, measure

the angles of the same stars: it is the same angle. Sitting in my

study here, I glance out of the window and discern separate bricks,

in houses five hundred feet away, with my unaided eye; they subtend

a discernible angle. But one thousand feet away I cannot distinguish

individual bricks; their width, being only two inches, does not

subtend an angle apprehensible to my vision. So at these distant

stars the earth's enormous orbit, if lying like a blazing ring in

space, with the world set on its edge like a pearl, and the sun

blazing like a diamond in the centre, would all shrink to a mere

point. Not quite to a point from the nearest stars, or we should

never be able to measure the distance of any of them. Professor Airy

says that our orbit, seen from the nearest star, would be the same

as a circle six-tenths of an inch in diameter seen at the distance

of a mile: it would all be hidden by a thread one-twenty-fifth of an

inch in diameter, held six hundred and fifty feet from the eye. If a

straight line could be drawn from a star, Sirius in the east to the

star Vega in the west, touching our [Page 71] earth's orbit on one

side, as T R A (Fig. 28), and a line were to be drawn six months

later from the same stars, touching our earth's orbit on the other

side, as R B T, such a line would not diverge sufficiently from a

straight line for us to detect its divergence. Numerous vain

attempts had been made, up to the year 1835, to detect and measure

the angle of parallax by which we could rescue some one or more of

the stars from the inconceivable depths of space, and ascertain

their distance from us. We are ever impelled to triumph over what is

declared to be unconquerable. There are peaks in the Alps no man has

ever climbed. They are assaulted every year by men zealous of more

worlds to conquer. So these greater heights of the heavens have been

assaulted, till some ambitious spirits have outsoared even

imagination by the certainties of mathematics.

[Illustration: Fig. 28.]

It is obvious that if one star were three times as far from us as

another, the nearer one would seem to be displaced by our movement

in our orbit three times as much as the other; so, by comparing one

star with another, we reach a ground of judgment. The ascertainment

of longitude at sea by means of the moon affords a good illustration.

Along the track where the moon sails, nine bright stars, four planets,

and the sun have been selected. The nautical almanacs give the

distance of the moon from these successive stars every hour in

the night for three years in advance. The sailor can measure the

distance at any time by his sextant. Looking from the world at

D (Fig. 29), the distance of the moon and [Page 72] star is A E,

which is given in the almanac. Looking from C, the distance is only

B E, which enables even the uneducated sailor to find the distance,

C D, on the earth, or his distance from Greenwich.

[Illustration: Fig. 29.--Mode of Ascertaining Longitude.]

So, by comparisons of the near and far stars, the approximate distance

of a few of them has been determined. The nearest one is the brightest

star in the Centaur, never visible in our northern latitudes, which

has a parallax of about one second. The next nearest is No. 61 in

the Swan, or 61 Cygni, having a parallax of 0".34. Approximate

measurements have been made on Sirius, Capella, the Pole Star,

etc., about eighteen in all. The distances are immense: only the

swiftest agents can traverse them. If our earth were suddenly to

dissolve its allegiance to the king of day, and attempt a flight

to the North Star, and should maintain its flight of one thousand

miles a minute, it would flyaway toward Polaris for thousands upon

thousands of years, till a million years had passed away, before

it reached that northern dome of the distant sky, and gave its

new allegiance to another sun. The sun it had left behind it would

gradually diminish till it was small as Arcturus, then small as

could be discerned by the naked eye, until at last it would finally

fade out in utter darkness long before the new sun was reached.

Light can traverse the distance around our earth eight times in

one second. It comes in eight minutes from the sun, but it takes

three and a quarter years to come from Alpha [Page 73] Centauri,

seven and a quarter years from 61 Cygni, and forty-five years from

the Polar Star.

Sometimes it happens that men steer along a lee shore, dependent

for direction on Polaris, that light-house in the sky. Sometimes it

has happened that men have traversed great swamps by night when that

star was the light-housse of freedom. In either case the exigency

of life and liberty was provided for forty-five years before by a

Providence that is divine.

We do not attempt to name in miles these enormous distances; we

must seek another yard-stick. Our astronomical unit and standard of

measurement is the distance of the earth from the sun--92,500,000

miles. This is the golden reed with which we measure the celestial

city. Thus, by laying down our astronomical unit 226,000 times, we

measure to Alpha Centauri, more than twenty millions of millions

of miles. Doubtless other suns are as far from Alpha Centauri and

each other as that is from ours.

Stars are not near or far according to their brightness. 61 Cygni is

a telescopic star, while Sirius, the brightest star in the heavens,

is twice as far away from us. One star differs from another star

in intrinsic glory.

The highest testimonies to the accuracy of these celestial observations

are found in the perfect predictions of eclipses, transits of planets

over the sun, occultation of stars by the moon, and those statements

of the Nautical Almanac that enable the sailor to know exactly

where he is on the pathless ocean by the telling of the stars:

"On the trackless ocean this book is the mariner's trusted friend

and counsellor; daily and nightly its revelations bring safety

to ships in all parts of the [Page 74] world. It is something more

than a mere book; it is an ever-present manifestation of the order

and harmony of the universe."

Another example of this wonderful accuracy is found in tracing

the asteroids. Within 200,000,000 or 300,000,000 miles from the

sun, the one hundred and ninety-two minute bodies that have been

already discovered move in paths very nearly the same--indeed two of

them traverse the same orbit, being one hundred and eighty degrees

apart;--they look alike, yet the eye of man in a few observations

so determines the curve of each orbit, that one is never mistaken

for another. But astronomy has higher uses than fixing time,

establishing landmarks, and guiding the sailor. It greatly quickens

and enlarges thought, excites a desire to know, leads to the utmost

exactness, and ministers to adoration and love of the Maker of

the innumerable suns.

[Page 75]

V.

Recreations in Astronomy With Directions for Practical Experiments and Telescopic Work · 第 11 / 38 题