Speaking generally, and neglecting all the complexities which delight

the soul of the astronomer, this is Delisle’s method of utilising a

transit. It has obviously one serious disadvantage as compared with

the other. An observer at one side of the earth has to bring his

observations into comparison with those made by an observer at the

other side of the earth. Each uses the local time of the place at which

he observes, and it has been calculated that for the result to be of

value there must not be an error of a single second in their estimates

of local time. Now, does the reader appreciate the full force of this

proviso? Each observer must know so certainly in what exact longitude

he is, that his estimate of the time when true noon occurs shall not be

one second wrong! This is all satisfactory enough in places where there

are regular observatories. But matters are changed when we are dealing

with such places as Woahoo, Kerguelen Land, Chatham Island, and the

wilds of Siberia.

In the transit[3] of 1874 there are many such difficulties to be

encountered. In fact, it is almost impossible to conceive a transit

the circumstances of which are more inconvenient. On the other hand,

however, the transit is of such a nature that if once the preliminary

difficulties are overcome, we can hope more from its indications than

from those of any other transit which will happen in the course of the

next few centuries.

The transit will begin earliest for observers in the neighbourhood

of the Sandwich Islands, latest for observers near Crozet Island,

far to the south-east of the Cape of Good Hope. It ends earliest for

observers far to the south-west of Cape Horn, latest for observers in

the north-eastern part of European Russia. Thus we see that, so far as

the application of our second method is concerned, the suitable spots

are not situated in the most inviting regions of the earth’s surface.

As the transit happens on December 8, 1874, the principal northern

stations will be very bleak abodes for the observers. The southern

stations are in yet more dreary regions,—notwithstanding the fact that

the transit occurs during the summer of the southern hemisphere.

For the application of Halley’s method we require stations where

the whole transit will be visible; and as the days are very short

at the northern stations in December, it is as respects these that

we encounter most difficulty. However, it has been found that many

places in Northern China, Japan, Eastern Siberia, and Manchouria are

suitable for the purpose. The best southern stations for this method

lie unfortunately on the unexplored Antarctic continent and the islands

adjacent to it; but Crozet Island, Kerguelen Land, and some other

places more easy of access than the Antarctic continent, will serve

very well. Indeed, England has so many stations to occupy elsewhere

that it is doubtful whether she will care to undertake the dangerous

and difficult task of exploring the Antarctic wastes to secure the best

southern stations. The work may fairly be left to other nations, and

doubtless will be efficiently carried out.

What England will actually undertake has not yet been fully decided

upon. We may be quite certain that she will send out a party to Woahoo

or Hawaii to observe the accelerated commencement of the transit.

She will also send observers to watch the retarded commencement, but

whether to Crozet Island, Kerguelen Land, Mauritius, or Rodriguez is

uncertain. Possibly two parties will be sent out for this purpose, and

most likely Rodriguez and Mauritius will be the places selected. It

had been thought until lately that the sun would be too low at some of

the places when the transit begins, but a more exact calculation of

the circumstances of the transit has shown this to be a mistake. Both

Crozet Island and Kerguelen Land are very likely to be enveloped in

heavy mists when the transit begins—that is, soon after sunrise—hence

the choice of Mauritius and Rodriguez as the most suitable station.

England will also be called on to take an important part in observing

the accelerated end of the transit. A party will probably be sent to

Chatham Island or Campbell Island, not far from New Zealand. It had

been thought that at the former island the sun would be too low; but

here, again, a more exact consideration of the circumstances of the

transit has led astronomers to the conclusion that the sun will be

quite high enough at this station.

The Russian observers are principally concerned with the observation

of the retarded end of the transit, nearly all the best stations lying

in Siberia. But there are several stations in British India where

this phase can be very usefully observed; and doubtless the skilful

astronomers and mathematicians who are taking part in the survey of

India will be invited—as at the time of the great eclipse—to give their

services in the cause of science. Alexandria, also, though inferior

to several of the Indian stations, will probably be visited by an

observing party from England.

It will be seen that England will thus be called on to supply about

half-a-dozen expeditions to view the transit. All of these will be sent

out in pursuance of Delisle’s mode of utilising a transit, so that, for

reasons already referred to, it will be necessary that they should be

provided with instruments of the utmost delicacy, and very carefully

constructed.[4] They will have to remain at their several stations for

a long time before the transit takes place—several months, at least—so

that they may accurately determine the latitude of the temporary

observatories they will erect. This is a work requiring skilled

observers and recondite processes of calculation. Hence it is that the

cost of sending out these observing parties is so considerable.

The only English party which will apply Halley’s method of observation

is the one which will be stationed at Mauritius, under Lord Lindsay.

This part of their work will be comparatively easy, the method only

requiring that the duration of the transit should be carefully

timed. In fact, one of the great advantages of Halley’s method is

the smallness of the expense it involves. A party might land the day

before the transit, and sail away the day after, with results at

least as trustworthy as those which a party applying Delisle’s method

could obtain after several months of hard work. It is to this, rather

than any other cause, that the small expense of the observations

made in 1769 is to be referred. And doubtless had it been decided

by our astronomical authorities to apply Halley’s method solely or

principally, the expense of the transit-observations would have been

materially lessened. There would, however, have been a risk of failure

through the occurrence of bad weather at the critical stations; whereas

now—as other nations will doubtless avail themselves of Halley’s

method—the chance that the transit-observations will fail through

meteorological causes is very largely diminished. Science will owe much

to the generosity of England in this respect.

It is, indeed, only recently that the possibility of applying Halley’s

method has been recognised. It had been thought that the method must

fail totally in 1874. But on a more careful examination of the

circumstances of the transit, a French astronomer, M. Puiseux, was

enabled to announce that this is not the case. Almost simultaneously I

published calculations pointing to a similar result; but having carried

the processes a few steps further than M. Puiseux, I was able to show

that Halley’s method is not only available in 1874, but is the more

powerful method of the two.

Unfortunately, there is an element of doubt in the inquiry, of which

no amount of care on the part of our observers and mathematicians will

enable them to get rid. I refer to the behaviour of Venus herself. It

is to the peculiarity we are now to consider that the _quasi_-failure

of the observations made in 1769 must be attributed. It is true that

Mr. Stone, the first-assistant at the Greenwich Observatory, has

managed to remove the greater part of the doubts which clouded the

results of those observations. But not even his skill and patience can

serve to remove the blot which a century of doubt has seemed to throw

upon the most exact of the sciences. We shall now show how much of the

blame of that unfortunate century of doubt is to be ascribed to Venus.

At a transit, astronomers confine their attention to one particular

phase—the moment, namely, when Venus just seems to lie wholly within

the outline of the sun’s disc. This at least was what Halley and

Delisle both suggested as desirable. Unfortunately, Venus had not

been consulted, and when the time of the transit came she declined

to enter upon or leave the sun’s face in the manner suggested by the

astronomers. Consider, for example, her conduct when entering on the

sun’s face:—

At first, as the black disc of the planet gradually notched the edge of

the sun’s disc, all seemed going on well. But when somewhat more than

half of the planet was on the sun’s face, it began to be noticed that

Venus was losing her rotundity of figure. She became gradually more and

more pear-shaped, until at last she looked very much like a peg-top

touching with its point the edge of the sun’s disc. Then suddenly—‘as

by a lightning flash,’ said one observer—the top lost its peg, and then

gradually Venus recovered her figure, and the transit proceeded without

further change on her part until the time came for her to leave the

sun’s face, when similar peculiarities took place in a reversed order.

Here was a serious difficulty indeed. For when was the moment of true

contact? Was it when the peg-top figure seemed just to touch the edge

of the sun? This seemed unlikely, because a moment after the planet

was seen well removed from the sun’s edge. Was it when the rotund part

of the planet belonged to a figure which would have touched the sun’s

edge if the rotundity had been perfect elsewhere? This, again, seemed

unlikely, because at this moment the black band connecting Venus and

the sun was quite wide. And, besides, if this were the true moment of

contact, what eye could be trusted to determine the occurrence of a

relation so peculiar? Yet the interval between this phase and the final

or peg-top phase lasted several seconds—as many as twenty-two in one

instance in 1769—and the whole success of the observation depended on

exactness within three or four seconds at the outside.

We know that Venus will act in precisely the same manner in 1874. If

we had been induced to hope that improvements in our telescopes would

diminish the peculiarity, the observations of the transit of Mercury,

in November 1868, would have sufficed to destroy that hope, for even

with the all but perfect instruments of the Greenwich Observatory,

Mercury assumed the peg-top disguise in the most unpleasing manner.

It may be asked, then, What do astronomers propose to do in 1874 to

prevent Venus from misleading them again as she did in 1769? Much has

already been done towards this end. Mr. Stone undertook a series of

careful researches to determine the law according to which Venus may be

expected to behave, or to misbehave herself; and the result is, that he

has been able to tell the observers exactly what they will have to look

for, and exactly what it is most important that they should record. In

1769, observers recorded their observations in such doubtful terms,

owing to their ignorance of the real significance of the peculiarities

they witnessed, that the mathematicians who had to make use of those

observations were misled. _Hinc illæ lacrymæ._ Hence it is that an

undeserved reproach has fallen upon the ‘exact science.’

The amount of the error resulting from the misinterpretation of the

observations made in 1769 was, however, very small indeed, when its

true character is considered. It is, indeed, easy to make the error

seem enormous. The sun’s distance came out some four millions of miles

too large, and that seems no trifling error. Then, again, the resulting

estimate of the distance of Neptune came out more than a hundred

million miles too great; while even this enormous error was as nothing

when compared with that which resulted when the distances of the fixed

stars were considered.

But this is an altogether erroneous mode of estimating the effect of

the error. It would be as absurd to count up the number of hairs’

breadth by which the geographer’s estimates of the length and breadth

of England may be in error. In all such matters it is relative and not

absolute error we have to consider. A microscopist would have made a

bad mistake who should over-estimate the length of a fly’s proboscis

by a single hair’s breadth; but the astronomer had made a wonderfully

successful measurement of the sun’s distance who deduced it within

three or four millions of miles of the true value. For it is readily

calculable that the error in the estimated relative bearing of the sun

as seen from opposite sides of the earth corresponds to the angle which

a hair’s breadth subtends when seen from a distance of 125 feet.

The error was first detected when other modes of determining the sun’s

distance were applied by the skilful astronomers and physicists of

our own day. We have no space to describe as fully as they deserve

the ingenious processes by which the great problem has been attacked

without aid from Venus. Indeed, we can but barely mention the

principles on which those methods depend. But to the reader who takes

interest in astronomy, we can recommend no subject as better worth

studying than the masterly researches of Foucault, Leverrier, and

Hansen upon the problem of the sun’s distance.

The problem has been attacked in four several ways. First, the

tremendous velocity of light has been measured by an ingenious

arrangement of revolving mirrors; the result combined with the

known time occupied by light in travelling across the earth’s orbit

immediately gives the sun’s distance. Secondly, a certain irregularity

in the moon’s motion, due to the fact that she is most disturbed by the

sun when traversing that half of her path which is nearest to him, was

pressed into the service with similar results. Thirdly, an irregularity

in the earth’s motion, due to the fact that she circles around the

common centre of gravity of her own mass and the moon’s, was made a

means of attacking the problem. Lastly, Mars, a planet which, as we

have already mentioned, approaches us almost as nearly as Venus, was

found an efficient ally.

The result of calculations founded on these methods showed that the

sun’s distance, instead of being about 95,000,000 miles, is little

more than 91,500,000 miles. And recently a re-examination of the

observations made upon Venus in 1769 led Mr. Stone to believe that they

point to a similar result.

Doubtless, however, we must wait for the transit of Venus in 1874

before forming a final decision as to the estimate of the sun’s

distance which is to take its place in popular works on astronomy

during the next century or so. Nothing but an unlooked-for combination

of unfavourable circumstances can cause the failure of our hopes.

Certainly, if we should fail in obtaining satisfactory results in 1874,

the world will not say that the generosity of the English Government

has been in fault, since it would be difficult to find a parallel in

the history of modern science to the munificence of the grant which

has been made this year for expeditions to observe a phenomenon whose

interest and importance are purely scientific.

(From _St. Paul’s_, October 1869.)

FOOTNOTES:

[3] The reader will remember the time at which the essay appeared. For

several reasons it seems well to leave the essay unaltered. In the

second series of Light Science a later stage is presented, and the

account is carried up to the present date in my work on _The Transits

of Venus_.

[4] It is held to be of the utmost importance that all the observing

parties should use similar telescopes.

_BRITAIN’S COAL CELLARS._

It would have been deemed a strange thought in the days of the Tudors

to suggest that England’s greatness would one day depend,—or seem to

depend,—on her stores of coal, a mineral then regarded as only an

unpleasant rival of the wood-log for household fires. When Shakespeare

put into the mouth of Faulconbridge the words—

This England never did, nor never shall,

Lie at the proud foot of a conqueror,

But when it first did help to wound itself,

he would have thought it a singular proviso that England should be

watchful of her coal stores if she would preserve her position among

the nations. And yet there is a closer connection between the present

greatness of Britain and the mighty coal cellars underlying certain

British counties than we are commonly prepared to acknowledge. Saxon

steadiness and Norman energy have doubtless played their part in

placing Britain in the position she now holds; but whatever may have

been the case in past ages of our history, it is certain that at

present there is much truth in Liebig’s assertion that England’s power

is in her coal. The time may come again, as the time has been, when we

shall be less dependent on our coal stores,—when bituminous bankruptcy

will not be equivalent to national bankruptcy; but if all our coal

mines were at this moment rendered unworkable, the power of England

would receive a shock from which it would be ages in recovering.

I have quoted an assertion made many years since by Baron Liebig. The

assertion was accompanied by another not less striking. ‘Civilisation,’

he said, ‘is the economy of power; and English power is coal.’ It is

on this text that I propose now to comment. There has recently been

issued a Blue Book, bearing in the most important manner on the subject

of England’s coal-supply. For five years fifteen eminent Commissioners

have been engaged in examining the available evidence respecting the

stores of coal contained in the various coal-fields of Great Britain.

Their inquiries were commenced soon after the time when the fears of

the country on this subject were first seriously awakened; and were

directed specially to ascertain how far those fears were justified

by the real circumstances of the case. It will be well to compare

the various opinions which were expressed before the inquiries were

commenced, with the results which have now been obtained.

In the first place it should be noticed that the subject had attracted

the attention of men of science many years ago. Some forty years[5]

have passed since Dr. Buckland, in one of the Bridgewater Treatises,

pointed to the necessity for a careful examination of our coal stores,

lest England should drift unawares into what he called ‘bituminous

bankruptcy.’ At that time the quantity of coal raised annually in

England amounted to but about forty millions of tons. Ten years later

the annual yield had risen to about fifty millions of tons; and then

another warning voice was raised by Dr. Arnold. Ten more years passed,

and the annual yield had increased to 83,635,214 tons, when Mr. Hull

made the startling announcement that our coal stores would last us but

about two centuries, unless some means were adopted to check the lavish

expenditure of our black diamonds.

But it was undoubtedly the address of Sir W. Armstrong to the British

Association, in 1863, which first roused the attention of the country

to the importance of the subject. ‘The greatness of England,’ he said,

‘depends much upon the superiority of her coal, in cheapness and

quality, over that of other nations. But we have already drawn from our

choicest mines a far larger quantity of coal than has been raised in

all other parts of the world put together; and the time is not remote

when we shall have to encounter the disadvantages of increased cost

of working and diminished value of produce.’ Then he summed up the

state of the case as he viewed it. ‘The entire quantity of available

coal existing in these islands has been calculated to amount to 80,000

millions of tons, which, at the present rate of consumption, would be

exhausted in 930 years; but with a continued yearly increase of 2¾

millions of tons would only last 212 years.’

Other statements were not wanting, however, which presented matters in

a more favourable light. Mr. Hussey Vivian, M.P., expressed the opinion

that South Wales alone could supply all England with coals for 500

years. Mr. R. C. Taylor, of the Geological Society, said that our coal

stores would suffice for 1,700 years. And there were some who adopted a

yet more sanguine view of our position.

Light Science for Leisure Hours A series of familiar essays on scientific subjects, natural phenomena, &c. · 第 4 / 19 段