How happens it, after such exact observations, that few astronomers now

admit the existence of active volcanoes in the moon? I will explain this

singularity in a few words.

The various parts of our satellite are not all equally reflecting. Here,

it may depend on the form, elsewhere, on the nature of the materials.

Those persons who have examined the moon with telescopes, know how very

considerable the difference arising from these two causes may be, how

much brighter one point of the moon sometimes is than those around it.

Now, it is quite evident that the relations of intensity between the

faint parts and the brilliant parts must continue to exist, whatever be

the origin of the illuminating light. In the portion of the lunar globe

that is illuminated by the sun, there are, everybody knows, some points,

the brightness of which is extraordinary compared to those around them;

those same points, when they are seen in that portion of the moon that

is only lighted by the earth, or in the ash-coloured part, will still

predominate over the neighbouring regions by their comparative

intensity. Thus we may explain the observations of the Slough

astronomer, without recurring to volcanoes. Whilst the great observer

was studying in the non-illuminated portion of the moon, the supposed

volcano of the 20th of April, 1787, his nine-foot telescope showed him

in truth, by the aid of the secondary rays proceeding from the earth,

even the darkest spots.

Herschel did not recur to the discussion of the supposed actually

burning lunar volcanoes, until 1791. In the volume of the _Philosophical

Transactions_ for 1792, he relates that, in directing a twenty-foot

telescope, magnifying 360 times, to the entirely eclipsed moon on the

22d of October, 1790, there were visible, over the whole face of the

satellite, about a hundred and fifty very luminous red points. The

author declares that he will observe the greatest reserve relative to

the similarity of all these points, their great brightness, and their

remarkable colour.

Yet is not red the usual colour of the moon when eclipsed, and when it

has not entirely disappeared? Could the solar rays reaching our

satellite by the effect of refraction, and after an absorption

experienced in the lowest strata of the terrestrial atmosphere, receive

another tint? Are there not in the moon, when freely illuminated, and

opposite to the sun, from one to two hundred little points, remarkable

by the brightness of their light? Would it be possible for those little

points not to be also distinguishable in the moon, when it receives only

the portion of solar light which is refracted and coloured by our

atmosphere?

Herschel was more successful in his remarks on the absence of a lunar

atmosphere. During the solar eclipse of the 5th September, 1793, the

illustrious astronomer particularly directed his attention to the shape

of the acute horn resulting from the intersection of the limbs of the

moon and of the sun. He deduced from his observation that if towards the

point of the horn there had been a deviation of only one second,

occasioned by the refraction of the solar light in the lunar atmosphere,

it would not have escaped him.

Herschel made the planets the object of numerous researches. Mercury was

the one with which he least occupied himself; he found its disk

perfectly round on observing it during its projection, that is to say,

in astronomical language, during its transit over the sun on the 9th of

November, 1802. He sought to determine the time of the rotation of Venus

since the year 1777. He published two memoirs relative to Mars, the one

in 1781, the other in 1784, and the discovery of its being flattened at

the poles we owe to him. After the discovery of the small planets,

Ceres, Pallas, Juno, and Vesta, by Piazzi, Olbers, and Harding, Herschel

applied himself to measuring their angular diameter. He concluded from

his researches that those four new bodies did not deserve the name of

planets, and he proposed to call them asteroïds. This epithet was

subsequently adopted; though bitterly criticized by a historian of the

Royal Society of London, Dr. Thomson, who went so far as to suppose

that the learned astronomer "had wished to deprive the first observers

of those bodies, of all idea of rating themselves as high as him

(Herschel) in the scale of astronomical discoverers." I should require

nothing farther to annihilate such an imputation, than to put it by the

side of the following passage, extracted from a memoir by this

celebrated astronomer, published in the _Philosophical Transactions_,

for the year 1805: "The specific difference existing between planets and

asteroïds appears now, by the addition of a third individual of the

latter species, to be more completely established, and that

circumstance, in my opinion, has added more to the _ornament_ of our

system than the discovery of a new planet could have done."

Although much has not resulted from Herschel's having occupied himself

with the physical constitution of Jupiter, astronomy is indebted to him

for several important results relative to the duration of that planet's

rotation. He also made numerous observations on the intensities and

comparative magnitudes of its satellites.

The compression of Saturn, the duration of its rotation, the physical

constitution of this planet and that of its ring, were, on the part of

Herschel, the object of numerous researches which have much contributed

to the progress of planetary astronomy. But on this subject two

important discoveries especially added new glory to the great

astronomer.

Of the five known satellites of Saturn at the close of the 17th century,

Huygens had discovered the fourth; Cassini the others.

The subject seemed to be exhausted, when news from Slough showed what a

mistake this was.

On the 28th of August, 1789, the great forty-foot telescope revealed to

Herschel a satellite still nearer to the ring than the other five

already observed. According to the principles of the nomenclature

previously adopted, the small body of the 28th August ought to have been

called the first satellite of Saturn, the numbers indicating the places

of the other five would then have been each increased by a unity. But

the fear of introducing confusion into science by these continual

changes of denomination, induced a preference for calling the new

satellite the sixth.

Thanks to the prodigious powers of the forty-foot telescope, a last

satellite, the seventh, showed itself on the 17th of September, 1789,

between the sixth and the ring.

This seventh satellite is extremely faint. Herschel, however, succeeding

in seeing it whenever circumstances were very favourable, even by the

aid of the twenty-foot telescope.

The discovery of the planet Uranus, the detection of its satellites,

will always occupy one of the highest places among those by which modern

astronomy is honoured.

On the 13th of March, 1781, between ten and eleven o'clock at night,

Herschel was examining the small stars near H Geminorum with a

seven-foot telescope, bearing a magnifying power of 227 times. One of

these stars seemed to him to have an unusual diameter. The celebrated

astronomer, therefore, thought it was a comet. It was under this

denomination that it was then discussed at the Royal Society of London.

But the researches of Herschel and of Laplace showed later that the

orbit of the new body was nearly circular, and Uranus was elevated to

the rank of a planet.

The immense distance of Uranus, its small angular diameter, the

feebleness of its light, did not allow the hope, that if that body had

satellites, the magnitudes of which were, relatively to its own size,

what the satellites of Jupiter, of Saturn are, compared to those two

large planets, any observer could perceive them, from the earth.

Herschel was not a man to be deterred by such discouraging conjectures.

Therefore, since powerful telescopes of the ordinary construction, that

is to say, with two mirrors conjugated, had not enabled him to discover

any thing, he substituted, in the beginning of January, 1787, _front

view_ telescopes, that is, telescopes throwing much more light on the

objects, the small mirror being then suppressed, and with it one of the

causes of loss of light is got rid of.

By patient labour, by observations requiring a rare perseverance,

Herschel attained (from the 11th of January, 1787, to the 28th of

February, 1794,) to the discovery of the six satellites of his planet,

and thus to complete the _world_ of a system that belongs entirely to

himself.

There are several of Herschel's memoirs on comets. In analyzing them, we

shall see that this great observer could not touch any thing without

making further discoveries in the subject.

Herschel applied some of his fine instruments to the study of the

physical constitution of a comet discovered by Mr. Pigott, on the 28th

September, 1807.

The nucleus was round and well determined. Some measures taken on the

day when the nucleus subtended only an angle of a single second, gave as

its real angle 6/100 of the diameter of the earth.

Herschel saw no phase at an epoch when only 7/10 of the nucleus could

be illuminated by the sun. The nucleus then must shine by its own light.

This is a legitimate inference in the opinion of every one who will

allow, on one hand, that the nucleus is a solid body, and on the other,

that it would have been possible to observe a phase of 8/10 on a disk

whose apparent total diameter did not exceed one or two seconds of a

degree.

Very small stars seemed to grow much paler when they were seen through

the coma or through the tail of the comet.

This faintness may have only been apparent, and might arise from the

circumstance of the stars being then projected on a luminous background.

Such is, indeed, the explanation adopted by Herschel. A gaseous medium,

capable of reflecting sufficient solar light to efface that of some

stars, would appear to him to possess in each stratum a sensible

quantity of matter, and to be, for that reason, a cause of real

diminution of the light transmitted, though nothing reveals the

existence of such a cause.

This argument, offered by Herschel in favour of the system which

transforms comets into self-luminous bodies, has not, as we may

perceive, much force. I might venture to say as much of many other

remarks by this great observer. He tells us that the comet was very

visible in the telescope on the 21st of February, 1808; now, on that

day, its distance from the sun amounted to 2.7 times the mean radius of

the terrestrial orbit; its distance from the observer was 2.9: "What

probability would there be that rays going to such distances, from the

sun to the comet, could, after their reflection, be seen by an eye

nearly three times more distant from the comet than from the sun?"

It is only numerical determinations that could give value to such an

argument. By satisfying himself with vague reasoning, Herschel did not

even perceive that he was committing a great mistake by making the

comet's distance from the observer appear to be an element of

visibility. If the comet be self-luminous, its intrinsic splendour (its

brightness for unity of surface) will remain constant at any distance,

as long as the subtended angle remains sensible. If the body shines by

borrowed light, its brightness will vary only according to its change of

distance from the sun; nor will the distance of the observer occasion

any change in the visibility; always, let it be understood, with the

restriction that the apparent diameter shall not be diminished below

certain limits.

Herschel finished his observations of a comet that was visible in

January, 1807, with the following remark:--

"Of the sixteen telescopic comets that I have examined, fourteen had no

solid body visible at their centre; the other two exhibited a central

light, very ill defined, that might be termed a nucleus, but a light

that certainly could not deserve the name of a disk."

The beautiful comet of 1811 became the object of that celebrated

astronomer's conscientious labour. Large telescopes showed him, in the

midst of the gazeous head, a rather reddish body of planetary

appearance, which bore strong magnifying powers, and showed no sign of

phase. Hence Herschel concluded that it was self-luminous. Yet if we

reflect that the planetary body under consideration was not a second in

diameter, the absence of a phase does not appear a demonstrative

argument.

The light of the head had a blueish-green tint. Was this a real tint, or

did the central reddish body, only through contrast, make the

surrounding vapour appear to be coloured? Herschel did not examine the

question in this point of view.

The head of the comet appeared to be enveloped at a certain distance, on

the side towards the sun, by a brilliant narrow zone, embracing about a

semicircle, and of a yellowish colour. From the two extremities of the

semicircle there arose, towards the region away from the sun, two long

luminous streaks which limited the tail. Between the brilliant circular

semi-ring and the head, the cometary substance seemed dark, very rare,

and very diaphanous.

The luminous semi-ring always presented similar appearances in all the

positions of the comet; it was not then possible to attribute to it

really the annular form, the shape of Saturn's ring, for example.

Herschel sought whether a spherical demi-envelop of luminous matter, and

yet diaphanous, would not lead to a natural explanation of the

phenomenon. In this hypothesis, the visual rays, which on the 6th of

October, 1811, made a section of the envelop, or bore almost

tangentially, traversed a thickness of matter of about 399,000

kilometres, (248,000 English miles,) whilst the visual rays near the

head of the comet did not meet above 80,000 kilometres (50,000 miles) of

it. As the brightness must be proportional to the quantity of matter

traversed, there could not fail to be an appearance around the comet, of

a semi-ring five times more luminous than the central regions. This

semi-ring, then, was an effect of projection, and it has revealed a

circumstance to us truly remarkable in the physical constitution of

comets.

The two luminous streaks that outlined the tail at its two limits, may

be explained in a similar manner; the tail was not flat as it appeared

to be; it had the form of a conoid, with its sides of a certain

thickness. The visual lines which traversed those sides almost

tangentially, evidently met much more matter than the visual lines

passing across. This maximum of matter could not fail of being

represented by a maximum of light.

The luminous semi-ring floated; it appeared one day to be suspended in

the diaphanous atmosphere by which the head of the comet was surrounded,

at a distance of 518,000 kilometres (322,000 English miles) from the

nucleus.

This distance was not constant. The matter of the semi-annular envelop

seemed even to be precipitated by slow degrees through the diaphanous

atmosphere; finally it reached the nucleus; the earlier appearances

vanished; the comet was reduced to a globular nebula.

During its period of dissolution, the ring appeared sometimes to have

several branches.

The luminous shreds of the tail seemed to undergo rapid, frequent, and

considerable variations of length. Herschel discerned symptoms of a

movement of rotation both in the comet and in its tail. This rotatory

motion carried unequal shreds from the centre towards the border, and

reciprocally. On looking from time to time at the same region of the

tail, at the border, for example, sensible changes of length must have

been perceptible, which however had no reality in them. Herschel

thought, as I have already said, that the beautiful comet of 1811, and

that of 1807, were self-luminous. The second comet of 1811 appeared to

him to shine only by borrowed light. It must be acknowledged that these

conjectures did not rest on any thing demonstrative.

In attentively comparing the comet of 1807 with the beautiful comet of

1811, relative to the changes of distance from the sun, and the

modifications resulting thence, Herschel put it beyond doubt that these

modifications have something individual in them, something relative to a

special state of the nebulous matter. On one celestial body the changes

of distance produce an enormous effect, on another the modifications are

insignificant.

OPTICAL LABOURS.

I shall say very little on the discoveries that Herschel made in

physics. In short, everybody knows them. They have been inserted into

special treatises, into elementary works, into verbal instruction; they

must be considered as the starting-point of a multitude of important

labours with which the sciences have been enriched during several years.

The chief of these is that of the dark radiating heat which is found

mixed with light.

In studying the phenomena, no longer with the eye, like Newton, but with

a thermometer, Herschel discovered that the solar spectrum is prolonged

on the red side far beyond the visible limits. The thermometer sometimes

rose higher in that dark region, than in the midst of brilliant zones.

The light of the sun then, contains, besides the coloured rays so well

characterized by Newton, some invisible rays, still less refrangible

than the red, and whose warming power is very considerable. A world of

discoveries has arisen from this fundamental fact.

The dark heat emanating from terrestrial objects more or less heated,

became also subjects of Herschel's investigations. His work contained

the germs of a good number of beautiful experiments since erected upon

it in our own day.

By successively placing the same objects in all parts of the solar

spectrum Herschel determined the illuminating powers of the various

prismatic rays. The general result of these experiments may be thus

enunciated:

The illuminating power of the red rays is not very great; that of the

orange rays surpasses it, and is in its turn surpassed by the power of

the yellow rays. The maximum power of illumination is found between the

brightest yellow and the palest green. The yellow and the green possess

this power equally. A like assimilation may be laid down between the

blue and the red. Finally, the power of illumination in the indigo rays,

and above all in the violet, is very weak.

Yet the memoirs of Herschel on Newton's coloured rings, though

containing a multitude of exact experiments, have not much contributed

to advance the theory of those curious phenomena. I have learnt from

good authority, that the great astronomer held the same opinion on this

topic. He said that it was the only occasion on which he had reason to

regret having, according to his constant method, published his labours

immediately, as fast as they were performed.

LAPLACE.

Having been appointed to draw up the report of a committee of the

Chamber of Deputies which was nominated in 1842, for the purpose of

taking into consideration the expediency of a proposal submitted to the

Chamber by the Minister of Public Instruction, relative to the

publication of a new edition of the works of Laplace at the public

expense, I deemed it to be my duty to embody in the report a concise

analysis of the works of our illustrious countryman. Several persons,

influenced, perhaps, by too indulgent a feeling towards me, having

expressed a wish that this analysis should not remain buried amid a heap

of legislative documents, but that it should be published in the

_Annuaire du Bureau des Longitudes_, I took advantage of this

circumstance to develop it more fully so as to render it less unworthy

of public attention. The scientific part of the report presented to the

Chamber of Deputies will be found here entire. It has been considered

desirable to suppress the remainder. I shall merely retain a few

sentences containing an explanation of the object of the proposed law,

and an announcement of the resolutions which were adopted by the three

powers of the State.

"Laplace has endowed France, Europe, the scientific world, with three

magnificent compositions: the _Traité de Mécanique Céleste_, the

_Exposition du Système du Monde_, and the _Théorie Analytique des

Probabilités_. In the present day (1842) there is no longer to be found

a single copy of this last work at any bookseller's establishment in

Paris. The edition of the _Mécanique Céleste_ itself will soon be

exhausted. It was painful then to reflect that the time was close at

hand when persons engaged in the study of the higher mathematics would

be compelled, for want of the original work, to inquire at Philadelphia,

at New York, or at Boston for the English translation of the _chef

d'oeuvre_ of our countryman by the excellent geometer Bowditch. These

fears, let us hasten to state, were not well founded. To republish the

_Mécanique Céleste_ was, on the part of the family of the illustrious

geometer, to perform a pious duty. Accordingly, Madame de Laplace, who

is so justly, so profoundly attentive to every circumstance calculated

to enhance the renown of the name which she bears, did not hesitate

about pecuniary considerations. A small property near Pont l'Evêque was

about to change hands, and the proceeds were to have been applied so

that Frenchmen should not be deprived of the satisfaction of exploring

the treasures of the _Mécanique Céleste_ through the medium of the

vernacular tongue.

"The republication of the complete works of Laplace rested upon an

equally sure guarantee. Yielding at once to filial affection, to a noble

feeling of patriotism, and to the enthusiasm for brilliant discoveries

which a course of severe study inspired, General Laplace had long since

qualified himself for becoming the editor of the seven volumes which are

destined to immortalize his father.

"There are glorious achievements of a character too elevated, of a

lustre too splendid, that they should continue to exist as objects of

private property. Upon the State devolves the duty of preserving them

from indifference and oblivion: of continually holding them up to

attention, of diffusing a knowledge of them through a thousand channels;

in a word, of rendering them subservient to the public interests.

"Doubtless the Minister of Public Instruction was influenced by these

considerations, when upon the occasion of a new edition of the works of

Laplace having become necessary, he demanded of you to substitute the

great French family for the personal family of the illustrious geometer.

We give our full and unreserved adhesion to this proposition. It springs

from a feeling of patriotism which will not be gainsayed by any one in

this assembly."

In fact, the Chamber of Deputies had only to examine and solve this

single question: "Are the works of Laplace of such transcendent, such

exceptional merit, that their republication ought to form the subject of

deliberation of the great powers of the State?" An opinion prevailed,

that it was not enough merely to appeal to public notoriety, but that it

was necessary to give an exact analysis of the brilliant discoveries of

Laplace in order to exhibit more fully the importance of the resolution

about to be adopted. Who could hereafter propose on any similar occasion

that the Chamber should declare itself without discussion, when a desire

was felt, previous to voting in favour of a resolution so honourable to

the memory of a great man, to fathom, to measure, to examine minutely

and from every point of view monuments such as the _Mécanique Céleste_

and the _Exposition du Système du Monde_? It has appeared to me that the

report drawn up in the name of a committee of one of the three great

powers of the State might worthily close this series of biographical

notices of eminent astronomers.[22]

The Marquis de Laplace, peer of France, one of the forty of the French

Academy, member of the Academy of Sciences and of the _Bureau des

Longitudes_, an associate of all the great Academies or Scientific

Societies of Europe, was born at Beaumont-en-Auge of parents belonging

to the class of small farmers, on the 28th of March, 1749; he died on

the 5th of March, 1827.

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