Having arrived at the fundamental principle that part of a lens

will act in a manner similar to a whole one, it is easy to explain

the construction of a heliometer. An ordinary telescope lens is

sawed in half by means of a thin round metal disk revolved rapidly

by machinery, and fed continually with emery and water at its

edge. The cutting effect of emery is sufficient to make such a

disk enter glass much as an ordinary saw penetrates wood. The two

"semi-lenses," as they are called, are then mounted separately in

metal holders. These are attached to one end of the heliometer,

called the "head," in such a way that the two semi-lenses can slide

side by side upon metal guides. This head is then fastened to one

end of a telescope tube mounted in the usual way. The "head" end

of the instrument is turned toward the sky in observing, and at

the eye-end is placed the usual little magnifier we have already

described.

The observer at the eye-end has control of certain rods by means

of which he can push the semi-lenses on their slides in the head

at the other end of the tube. Now, if he moves the semi-lenses so

as to bring them side by side exactly, the whole arrangement will

act like an ordinary telescope. For the semi-lenses will then fit

together just as if the original glass had never been cut. But

if the half-lenses are separated a little on their slides, each

will act by itself. Being slightly separated, each will cover a

different part of the sky. The whole affair acts as if the observer

at the eye-end were looking through two telescopes at once. For

each semi-lens acts independently, just as if it were a complete

glass of only half the size.

Now, suppose there were a couple of stars in the sky, one in the

part covered by the first semi-lens, and one in the part covered

by the second. The observer would, of course, see both stars at

once upon looking into the little magnifier at the eye-end of the

heliometer.

We must remember that these stars will appear in the field of view

simply as two tiny points of light. The astronomer, as we have

said, is provided with a simple system of long rods, by means of

which he can manipulate the semi-lenses while the observation is

being made. If he slides them very slowly one way or the other, the

two star-points in the field of view will be seen to approach each

other. In this way they can at last be brought so near together

that they will form but a single dot of light. Observation with

the heliometer consists in thus bringing two star-images together,

until at last they are superimposed one upon the other, and we see

one image only. Means are provided by which it is then possible to

measure the amount of separation of the two half-lenses. Evidently

the farther asunder on the sky are the two stars under observation,

the greater will be the separation of the semi-lenses necessary

to make a single image of their light. Thus, measurement of the

lenses' separation becomes a means of determining the separation

of the stars themselves upon the sky.

The two slides in the heliometer head are supplied with a pair of

very delicate measures or "scales" usually made of silver. These

can be examined from the eye-end of the instrument by looking

through a long microscope provided for this special purpose. Thus

an extremely precise value is obtained both of the separation of

the sliders and of the distance on the sky between the stars under

examination. Measures made in this way with the heliometer are

counted the most precise of astronomical observations.

Having thus described briefly the kind of observations obtained

with the heliometer, we shall now touch upon their further

utilization. We shall take as an example but one of their many

uses--that one which astronomers consider the most important--the

measurement of stellar distances. (See also p. 94.)

Even the nearest fixed star is almost inconceivably remote from

us. And astronomers are imprisoned on this little earth; we cannot

bridge the profound distance separating us from the stars, so as

to use direct measurement with tape-line or surveyor's chain. We

are forced to have recourse to some indirect method. Suppose a

certain star is suspected, on account of its brightness, or for

some other reason, of being near us in space, and so giving a

favorable opportunity for a determination of distance. A couple of

very faint stars are selected close by. These, on account of their

faintness, the astronomer may regard as quite immeasurably far

away. He then determines with his heliometer the exact position on

the sky of the bright star with respect to the pair of faint ones.

Half a year is then allowed to pass. During that time the earth has

been swinging along in its annual path or orbit around the sun.

Half a year will have sufficed to carry the observer on the earth

to the other side of that path, and he is then 185,000,000 miles

away from his position at the first observation.

Another determination is made of the bright star's position as

referred to the two faint ones. Now, if all these stars were

equally distant, their relative positions at the second observation

would be just the same as at the former one. But if, as is very

probable, the bright star is very much nearer us than are the two

faint ones, we shall obtain a different position from our second

observation. For the change of 185,000,000 miles in the observer's

location will, of course, affect the direction in which we see

the near star, while it will leave the distant ones practically

unchanged. Without entering into technical details, we may say that

from a large number of observations of this kind, we can obtain

the distance of the bright star by a process of calculation. The

only essential is to have an instrument that can make the actual

observations of position accurately enough; and in this respect the

heliometer is still unexcelled.

OCCULTATIONS

Scarcely anyone can have watched the sky without noticing how

different is the behavior of our moon from that of any other object

we can see. Of course, it has this in common with the sun and stars

and planets, that it rises in the eastern horizon, slowly climbs

the dome of the sky, and again goes down and sets in the west.

This motion of the heavenly bodies is known to be an apparent one

merely, and caused by the turning of our own earth upon its axis. A

man standing upon the earth's surface can look up and see above him

one-half the great celestial vault, gemmed with twinkling stars,

and bearing, perhaps, within its ample curve one or two serenely

shining planets and the lustrous moon. But at any given moment the

observer can see nothing of the other half of the heavenly sphere.

It is beneath his feet, and concealed by the solid bulk of the

earth.

The earth, however, is turning on an axis, carrying the observer

with it. And so it is continually presenting him to a new part of

the sky. At any moment he sees but a single half-sphere; yet the

very next instant it is no longer the same; a small portion has

passed out of sight on one side by going down behind the turning

earth, while a corresponding new section has come into view on

the opposite side. It is this coming into view that we call the

rising of a star; and the corresponding disappearance on the other

side is called setting. Thus rising and setting are, of course,

due entirely to a turning of the earth, and not at all to actual

motions of the stars; and for this reason, all objects in the sky,

without exception, must rise and set again. But the moon really has

a motion of its own in addition to this apparent one caused by the

earth's rotation.

Somewhere in the dawn of time early watchers of the stars thought

out those fancied constellations that survive even down to our own

day. They placed the mighty lion, king of beasts, upon the face

of night, and the great hunter, too, armed with club and dagger,

to pursue him. Among these constellations the moon threads her

destined way, night after night, so rapidly that the unaided eye

can see that she is moving. It needs but little power of fancy's

magic to recall from the dim past a picture of some aged astronomer

graving upon his tablets the Records of the Moon. "To-night she is

near the bright star in the eye of the Bull." And again: "To-night

she rides full, and near to the heart of the Virgin."

And why does the moon ride thus through the stars of night? Modern

science has succeeded in disentangling the intricacies of her

motion, until to-day only one or two of the very minutest details

of that motion remain unexplained. But it has been a hard problem.

Someone has well said that lunar theory should be likened to a

lofty cliff upon whose side the intellectual giants among men can

mark off their mental stature, but whose height no one of them may

ever hope to scale.

But for our present purpose it is unnecessary to pursue the subject

of lunar motion into its abstruser details. To understand why the

moon moves rapidly among the stars, it is sufficient to remember

that she is whirling quickly round the earth, so as to complete

her circuit in a little less than a month. We see her at all times

projected upon the distant background of the sky on which are set

the stellar points of light, as though intended for beacons to

mark the course pursued by moon and planets. The stars themselves

have no such motions as the moon; situated at a distance almost

inconceivably great, they may, indeed, be travellers through empty

space, yet their journeys shrink into insignificance as seen from

distant earth. It requires the most delicate instruments of the

astronomer to so magnify the tiny displacements of the stars on the

celestial vault that they may be measured by human eyes.

Let us again recur to our supposed observer watching the moon night

after night, so as to record the stars closely approached by her.

Why should he not some time or other be surprised by an approach so

close as to amount apparently to actual contact? The moon covers

quite a large surface on the sky, and when we remember the nearly

countless numbers of the stars, it would, indeed, be strange if

there were not some behind the moon as well as all around her.

A moment's consideration shows that this must often be the case;

and in fact, if the moon's advancing edge be scrutinized carefully

through a telescope, small stars can be seen frequently to

disappear behind it. This is a most interesting observation. At

first we see the moon and star near each other in the telescope's

field of view. But the distance between them lessens perceptibly,

even quickly, until at last, with a startling suddenness, the star

goes out of sight behind the moon. After a time, ranging from a few

moments to, perhaps, more than an hour, the moon will pass, and we

can see the star suddenly reappear from behind the other edge.

These interesting observations, while not at all uncommon, can

be made only very rarely by naked-eye astronomers. The reason is

simple. The moon's light is so brilliant that it fairly overcomes

the stars whenever they are at all near, except in the case of

very bright ones. Small stars that can be followed quite easily

up to the moon's edge in a good telescope, disappear from a

naked-eye view while the moon is still a long distance away. But

the number of very bright stars is comparatively small, so that

it is quite unusual to find anyone not a professional astronomer

who has actually seen one of these so-called "occultations."

Moreover, most people are not informed in advance of the occurrence

of an opportunity to make such observations, although they can be

predicted quite easily by the aid of astronomical calculations.

Sometimes we have occultations of planets, and these are the most

interesting of all. When the moon passes between us and one of the

larger planets, it is worth while to observe the phenomenon even

without a telescope.

Up to this point we have considered occultations chiefly as being

of interest to the naked-eye astronomer. Yet occultations have a

real scientific value. It is by their means that we can, perhaps,

best measure the moon's size. By noting with a telescope the time

of disappearance and reappearance of known stars, astronomers can

bring the direct measurement of the moon's diameter within the

range of their numerical calculations. Sometimes the moon passes

over a condensed cluster of stars like the Pleiades. The results

obtainable on these occasions are valuable in a very high degree,

and contribute largely to making precise our knowledge of the lunar

diameter.

There is another thing of scientific interest about occultations,

though it has lost some of its importance in recent years. When

such an event has been observed, the agreement of the predicted

time with that actually recorded by the astronomer offers a most

searching test of the correctness of our theory of lunar motion. We

have already called attention to the great inherent difficulty of

this theory. It is easy to see that by noting the exact instant of

disappearance of a star at a place on the earth the latitude and

longitude of which are known, we can both check our calculations

and gather material for improving our theory. The same principle

can be used also in the converse direction. Within the limits of

precision imposed by the state of our knowledge of lunar theory,

we can utilize occultations to help determine the position on

the earth of places whose longitude is unknown. It is a very

interesting bit of history that the first determination of the

longitude of Washington was made by means of occultations, and that

this early determination led to the founding of the United States

Naval Observatory.

On March 28, 1810, Mr. Pitkin, of Connecticut, reported to

the House of Representatives on "laying a foundation for the

establishment of a first meridian for the United States, by which a

further dependence on Great Britain or any other foreign nation for

such meridian may be entirely removed." This report was the result

of a memorial presented by one William Lambert, who had deduced the

longitude of the Capitol from an occultation observed October 20,

1804. Various proceedings were had in Congress and in committee,

until at last, in 1821, Lambert was appointed "to make astronomical

observations by lunar occultations of fixed stars, solar eclipses,

or any approved method adapted to ascertain the longitude of the

Capitol from Greenwich." Lambert's reports were made in 1822

and 1823, but ten years passed before the establishment of a

formal Naval Observatory under Goldsborough, Wilkes, and Gilliss.

But to Lambert belongs the honor of having marked out the first

fundamental official meridian of longitude in the United States.

MOUNTING GREAT TELESCOPES

There are many interesting practical things about an astronomical

observatory with which the public seldom has an opportunity to

become acquainted. Among these, perhaps, the details connected

with setting up a great telescope take first rank. The writer

happened to be present at the Cape of Good Hope Observatory when

the photographic equatorial telescope was being mounted, and the

operation of putting it in position may be taken as typical of

similar processes elsewhere. (See also p. 86.)

[Illustration: Forty-Inch Telescope, Yerkes Observatory, University

of Chicago.]

In the first place, it is necessary to explain what is meant by an

"equatorial" telescope. One of the chief difficulties in making

ordinary observations arises from the rising and setting of the

stars. They are all apparently moving across the face of the sky,

usually climbing up from the eastern horizon, only to go down again

and set in the west. If, therefore, we wish to scrutinize any

given object for a considerable time, we must move the telescope

continuously so as to keep pace with the motion of the heavens. For

this purpose, the tube must be attached to axles, so that it can be

turned easily in any direction. The equatorial mounting is a device

that permits the telescope to be thus aimed at any part of the sky,

and at the same time facilitates greatly the operation of keeping

it pointed correctly after a star has once been brought into the

field of view.

To understand the equatorial mounting it is necessary to remember

that the rising and setting motions of the heavenly bodies are

apparent ones only, and due in reality to the turning of the earth

on its own axis. As the earth goes around, it carries observer,

telescope, and observatory past the stars fixed upon the distant

sky. Consequently, to keep a telescope pointed continuously at a

given star, it is merely necessary to rotate it steadily backward

upon a suitable axis just fast enough to neutralize exactly the

turning of our earth.

By a suitable axis for this purpose we mean one so mounted as

to be exactly parallel to the earth's own axis of rotation. A

little reflection shows how simply such an arrangement will work.

All the heavenly bodies may be regarded, for practical purposes,

as excessively remote in comparison with the dimensions of our

earth. The entire planet shrinks into absolute insignificance

when compared with the distances of the nearest objects brought

under observation by astronomers. It follows that if we have our

telescope attached to such a rotation-axis as we have described,

it will be just the same for purposes of observation as though the

telescope's axis were not only parallel to the earth's axis, but

actually coincident with it. The two axes may be separated by a

distance equal to that between the earth's surface and its centre;

but, as we have said, this distance is insignificant so far as our

present object is concerned.

There is another way to arrive at the same result. We know that

the stars in rising and setting all seem to revolve about the pole

star, which itself seems to remain immovable. Consequently, if we

mount our telescope so that it can turn about an axis pointing at

the pole, we shall be able to neutralize the rotation of the stars

by simply turning the telescope about the axis at the proper speed

and in the right direction. Astronomical considerations teach us

that an axis thus pointing at the pole will be parallel to the

earth's own axis. Thus we arrive at the same fundamental principle

for mounting an astronomical telescope from whichever point of view

we consider the subject.

Every large telescope is provided with such an axis of rotation;

and for the reason stated it is called the "polar axis." The

telescope itself is then called an "equatorial." The advantage

of this method of mounting is very evident. Since we can follow

the stars' motions by turning the telescope about one axis only,

it becomes a very simple matter to accomplish this turning

automatically by means of clock-work.

The "following" of a star being thus provided for by the device

of a polar axis, it is, of course, also necessary to supply some

other motion so as to enable us to aim the tube at any point in the

heavens. For it is obvious that if it were rigidly attached to the

polar axis, we could, indeed, follow any star that happened to be

in the field of view, but we could not change this field of view at

will so as to observe other stars or planets. To accomplish this,

the telescope is attached to the polar axis by means of a pivot.

By turning the telescope around its polar axis, and also on this

pivot, we can find any object in the heavens; and once found, we

can leave to the polar axis and its automatic clock-work the task

of keeping that object before the observer's eye.

In setting up the Cape of Good Hope instrument the astronomers were

obliged to do a large part of the work of adjustment personally.

Far away from European instrument-makers, the parts of the

mounting and telescope had to be "assembled," or put together, by

the astronomers of the Cape Observatory. A heavy pier of brick

and masonry had been prepared in advance. Upon this was placed a

massive iron base, intended to support the superstructure of polar

axis and telescope. This base rested on three points, one of which

could be screwed in and out, so as to tilt the whole affair a

little forward or backward. By means of this screw we effected the

final adjustment of the polar axis to exact parallelism with that

of the earth. Other screws were provided with which the base could

be twisted a little horizontally either to the right or left. Once

set up in a position almost correct, it was easy to perfect the

adjustment by the aid of these screws.

Afterward the tube and lenses were put in place, and the clock

properly attached inside the big cast-iron base. This clock-work

looked more like a piece of heavy machinery than a delicate clock

mechanism. But it had heavy work to do, carrying the massive

telescope with its weighty lenses, and needed to be correspondingly

strong. It had a driving-weight of about 2,000 pounds, and was so

powerful that turning the telescope affected it no more than the

hour-hand of an ordinary clock affects the mechanism within its

case.

The final test of the whole adjustment consisted in noting whether

stars once brought into the telescopic field of view could be

maintained there automatically by means of the clock. This object

having been attained successfully, the instrument stood ready to be

used in the routine business of the observatory.

Before leaving the subject of telescope-mountings, we must mention

the giant instrument set up at the Paris Exposition of 1900. The

project of having a _Grande Lunette_ had been hailed by newspapers

throughout the world and by the general public in their customary

excitable way. It was tremendously over-advertised; exaggerated

notions of the instrument's powers were spread abroad and eagerly

credited; the moon was to be dragged down, as it were, from its

customary place in the sky, so near that we should be able almost

to touch its surface. As to the planets--free license was given to

the journalistic imagination, and there was no effective limitation

to the magnificence of astronomical discovery practically within

our grasp, beyond the necessity for printed space demanded by

sundry wars, pestilences, and other mundane trifles.

[Illustration: Yerkes Observatory, University of Chicago.]

Now, the present writer is very far from advocating a lessening of

the attention devoted to astronomy. Rather would he magnify his

office than diminish it. But let journalistic astronomy be as good

an imitation of sober scientific truth as can be procured at space

rates; let editors encourage the public to study those things

in the science that are ennobling and cultivating to the mind;

let there be an end to the frenzied effort to fabricate a highly

colored account of alleged discoveries of yesterday, capable of

masquerading to-day under heavy head-lines as News.

The manner in which the big telescope came to be built is not

without interest, and shows that enterprise is far from dead, even

in the old countries. A stock company was organized--we should

call it a corporation--under the name _Société de l'Optique_. It

would appear that shares were regularly put on the market, and

that a prospectus, more or less alluring, was widely distributed.

We may say at once that the investing public did not respond

with obtrusive alacrity; but at all events, the promoters'

efforts received sufficient encouragement to enable them to begin

active work. From the very first a vigorous attempt was made to

utilize both the resources of genuine science and the devices of

quasi-charlatanry. It was announced that the public were to be

admitted to look through the big glass (apparently at so much an

eye), and many, doubtless, expected that the man in the street

would be able to make personal acquaintance with the man in the

moon. A telescopic image of the sun was to be projected on a big

screen, and exhibited to a concourse of spectators assembled in

rising tiers of seats within a great amphitheatre. And when clouds

or other circumstances should prevent observing the planets or

scrutinizing the sun, a powerful stereopticon was to be used.

Artificial pictures of the wonders of heaven were to be projected

on the screen, and the public would never be disappointed. It

was arranged that skilled talkers should be present to explain

all marvels: and, in short, financial profit was to be combined

with machinery for advancing scientific discovery. Astronomers

the world over were "circularized," asked to become shareholders,

and, in default of that, to send lantern-slides or photographs of

remarkable celestial objects for exhibition in the magic-lantern

part of the show.

Practical Talks by an Astronomer · 第 7 / 10 段