CHAPTER VI.

GALILEI.

“Dans la Science nous sommes tous disciples de Galilée.”—TROUESSART.

“Bacon pointed out at a distance the road to true philosophy: Galileo

both pointed it out to others, and made himself considerable advances

in it.”—DAVID HUME.

113. To the generation which succeeded Tycho belonged two of the best

known of all astronomers, Galilei and Kepler. Although they were nearly

contemporaries, Galilei having been born seven years earlier than

Kepler, and surviving him by twelve years, their methods of work and

their contributions to astronomy were so different in character, and

their influence on one another so slight, that it is convenient to make

some departure from strict chronological order, and to devote this

chapter exclusively to Galilei, leaving Kepler to the next.

_Galileo Galilei_ was born in 1564, at Pisa, at that time in the Grand

Duchy of Tuscany, on the day of Michel Angelo’s death and in the year

of Shakespeare’s birth. His father, Vincenzo, was an impoverished

member of a good Florentine family, and was distinguished by his skill

in music and mathematics. Galileo’s talents shewed themselves early,

and although it was originally intended that he should earn his living

by trade, Vincenzo was wise enough to see that his son’s ability and

tastes rendered him much more fit for a professional career, and

accordingly he sent him in 1581 to study medicine at the University

of Pisa. Here his unusual gifts soon made him conspicuous, and he

became noted in particular for his unwillingness to accept without

question the dogmatic statements of his teachers, which were based not

on direct evidence, but on the authority of the great writers of the

past. This valuable characteristic, which marked him throughout his

life, coupled with his skill in argument, earned for him the dislike of

some of his professors, and from his fellow-students the nickname of

The Wrangler.

114. In 1582 his keen observation led to his first scientific

discovery. Happening one day in the Cathedral of Pisa to be looking at

the swinging of a lamp which was hanging from the roof, he noticed that

as the motion gradually died away and the extent of each oscillation

became less, the time occupied by each oscillation remained sensibly

the same, a result which he verified more precisely by comparison with

the beating of his pulse. Further thought and trial shewed him that

this property was not peculiar to cathedral lamps, but that any weight

hung by a string (or any other form of pendulum) swung to and fro

in a time which depended only on the length of the string and other

characteristics of the pendulum itself, and not to any appreciable

extent on the way in which it was set in motion or on the extent of

each oscillation. He devised accordingly an instrument the oscillations

of which could be used while they lasted as a measure of time, and

which was in practice found very useful by doctors for measuring the

rate of a patient’s pulse.

115. Before very long it became evident that Galilei had no special

taste for medicine, a study selected for him chiefly as leading to a

reasonably lucrative professional career, and that his real bent was

for mathematics and its applications to experimental science. He had

received little or no formal teaching in mathematics before his second

year at the University, in the course of which he happened to overhear

a lesson on Euclid’s geometry, given at the Grand Duke’s court, and

was so fascinated that he continued to attend the course, at first

surreptitiously, afterwards openly; his interest in the subject was

thereby so much stimulated, and his aptitude for it was so marked,

that he obtained his father’s consent to abandon medicine in favour of

mathematics.

In 1585, however, poverty compelled him to quit the University without

completing the regular course and obtaining a degree, and the next four

years were spent chiefly at home, where he continued to read and to

think on scientific subjects. In the year 1586 he wrote his first known

scientific essay,[66] which was circulated in manuscript, and only

printed during the present century.

116. In 1589 he was appointed for three years to a professorship

of mathematics (including astronomy) at Pisa. A miserable stipend,

equivalent to about five shillings a week, was attached to the post,

but this he was to some extent able to supplement by taking private

pupils.

In his new position Galilei had scope for his remarkable power

of exposition, but far from being content with giving lectures

on traditional lines he also carried out a series of scientific

investigations, important both in themselves and on account of the

novelty in the method of investigation employed.

It will be convenient to discuss more fully at the end of this chapter

Galilei’s contributions to mechanics and to scientific method, and

merely to refer here briefly to his first experiments on falling

bodies, which were made at this time. Some were performed by dropping

various bodies from the top of the leaning tower of Pisa, and others

by rolling balls down grooves arranged at different inclinations.

It is difficult to us nowadays, when scientific experiments are so

common, to realise the novelty and importance at the end of the 16th

century of such simple experiments. The mediaeval tradition of carrying

out scientific investigation largely by the interpretation of texts

in Aristotle, Galen, or other great writers of the past, and by the

deduction of results from general principles which were to be found in

these writers without any fresh appeal to observation, still prevailed

almost undisturbed at Pisa, as elsewhere. It was in particular commonly

asserted, on the authority of Aristotle, that, the cause of the fall of

a heavy body being its weight, a heavier body must fall faster than a

lighter one and in proportion to its greater weight. It may perhaps be

doubted whether any one before Galilei’s time had clear enough ideas

on the subject to be able to give a definite answer to such a question

as how much farther a ten-pound weight would fall in a second than a

one-pound weight; but if so he would probably have said that it would

fall ten times as far, or else that it would require ten times as long

to fall the same distance. To actually try the experiment, to vary

its conditions, so as to remove as many accidental causes of error as

possible, to increase in some way the time of the fall so as to enable

it to be measured with more accuracy, these ideas, put into practice by

Galilei, were entirely foreign to the prevailing habits of scientific

thought, and were indeed regarded by most of his colleagues as

undesirable if not dangerous innovations. A few simple experiments were

enough to prove the complete falsity of the current beliefs in this

matter, and to establish that in general bodies of different weights

fell nearly the same distance in the same time, the difference being

not more than could reasonably be ascribed to the resistance offered by

the air.

These and other results were embodied in a tract, which, like most of

Galilei’s earlier writings, was only circulated in manuscript, the

substance of it being first printed in the great treatise on mechanics

which he published towards the end of his life (§ 133).

These innovations, coupled with the slight respect that he was in the

habit of paying to those who differed from him, evidently made Galilei

far from popular with his colleagues at Pisa, and either on this

account, or on account of domestic troubles consequent on the death of

his father (1591), he resigned his professorship shortly before the

expiration of his term of office, and returned to his mother’s home at

Florence.

117. After a few months spent at Florence he was appointed, by the

influence of a Venetian friend, to a professorship of mathematics at

Padua, which was then in the territory of the Venetian republic (1592).

The appointment was in the first instance for a period of six years,

and the salary much larger than at Pisa. During the first few years

of Galilei’s career at Padua his activity seems to have been very

great and very varied; in addition to giving his regular lectures,

to audiences which rapidly increased, he wrote tracts, for the most

part not printed at the time, on astronomy, on mechanics, and on

fortification, and invented a variety of scientific instruments.

No record exists of the exact time at which he first adopted the

astronomical views of Coppernicus, but he himself stated that in 1597

he had adopted them some years before, and had collected arguments in

their support.

In the following year his professorship was renewed for six years with

an increased stipend, a renewal which was subsequently made for six

years more, and finally for life, the stipend being increased on each

occasion.

Galilei’s first contribution to astronomical discovery was made in

1604, when a star appeared suddenly in the constellation Serpentarius,

and was shewn by him to be at any rate more distant than the planets, a

result confirming Tycho’s conclusions (chapter V., § 100) that changes

take place in the celestial regions even beyond the planets, and are

by no means confined—as was commonly believed—to the earth and its

immediate surroundings.

118. By this time Galilei had become famous throughout Italy, not only

as a brilliant lecturer, but also as a learned and original man of

science. The discoveries which first gave him a European reputation

were, however, the series of telescopic observations made in 1609 and

the following years.

Roger Bacon (chapter III., § 67) had claimed to have devised a

combination of lenses enabling distant objects to be seen as if they

were near; a similar invention was probably made by our countryman

_Leonard Digges_ (who died about 1571), and was described also by the

Italian _Porta_ in 1558. If such an instrument was actually made by

any one of the three, which is not certain, the discovery at any rate

attracted no attention and was again lost. The effective discovery

of the telescope was made in Holland in 1608 by _Hans Lippersheim_

(?-1619), a spectacle-maker of Middleburg, and almost simultaneously by

two other Dutchmen, but whether independently or not it is impossible

to say. Early in the following year the report of the invention

reached Galilei, who, though without any detailed information as to

the structure of the instrument, succeeded after a few trials in

arranging two lenses—one convex and one concave—in a tube in such a

way as to enlarge the apparent size of an object looked at; his first

instrument made objects appear three times nearer, consequently three

times greater (in breadth and height), and he was soon able to make

telescopes which in the same way magnified thirty-fold.

That the new instrument might be applied to celestial as well as

to terrestrial objects was a fairly obvious idea, which was acted

on almost at once by the English mathematician _Thomas Harriot_

(1560-1621), by _Simon Marius_ (1570-1624) in Germany, and by Galilei.

That the credit of first using the telescope for astronomical

purposes is almost invariably attributed to Galilei, though his first

observations were in all probability slightly later in date than those

of Harriot and Marius, is to a great extent justified by the persistent

way in which he examined object after object, whenever there seemed any

reasonable prospect of results following, by the energy and acuteness

with which he followed up each clue, by the independence of mind with

which he interpreted his observations, and above all by the insight

with which he realised their astronomical importance.

119. His first series of telescopic discoveries were published early

in 1610 in a little book called _Sidereus Nuncius_, or _The Sidereal

Messenger_. His first observations at once threw a flood of light

on the nature of our nearest celestial neighbour, the moon. It was

commonly believed that the moon, like the other celestial bodies, was

perfectly smooth and spherical, and the cause of the familiar dark

markings on the surface was quite unknown.[67]

[Illustration: FIG. 53.—One of Galilei’s drawings of the moon. From the

_Sidereus Nuncius_.]

Galilei discovered at once a number of smaller markings, both bright

and dark (fig. 53), and recognised many of the latter as shadows of

lunar mountains cast by the sun; and further identified bright spots

seen near the boundary of the illuminated and dark portions of the moon

as mountain-tops just catching the light of the rising or setting sun,

while the surrounding lunar area was still in darkness. Moreover, with

characteristic ingenuity and love of precision, he calculated from

observations of this nature the height of some of the more conspicuous

lunar mountains, the largest being estimated by him to be about

four miles high, a result agreeing closely with modern estimates of

the greatest height on the moon. The large dark spots he explained

(erroneously) as possibly caused by water, though he evidently had

less confidence in the correctness of the explanation than some of his

immediate scientific successors, by whom the name of =seas= was given

to these spots (chapter VIII., § 153). He noticed also the absence of

clouds. Apart however from details, the really significant results of

his observations were that the moon was in many important respects

similar to the earth, that the traditional belief in its perfectly

spherical form had to be abandoned, and that so far the received

doctrine of the sharp distinction to be drawn between things celestial

and things terrestrial was shewn to be without justification; the

importance of this in connection with the Coppernican view that the

earth, instead of being unique, was one of six planets revolving round

the sun, needs no comment.

One of Galilei’s numerous scientific opponents[68] attempted to explain

away the apparent contradiction between the old theory and the new

observations by the ingenious suggestion that the apparent valleys

in the moon were in reality filled with some _invisible_ crystalline

material, so that the moon was in fact perfectly spherical. To this

Galilei replied that the idea was so excellent that he wished to extend

its application, and accordingly maintained that the moon had on it

mountains of this same invisible substance, at least ten times as high

as any which he had observed.

120. The telescope revealed also the existence of an immense number

of stars too faint to be seen by the unaided eye; Galilei saw, for

example, 36 stars in the Pleiades, which to an ordinary eye consist

of six only. Portions of the Milky Way and various nebulous patches

of light were also discovered to consist of multitudes of faint stars

clustered together; in the cluster Præsepe (in the Crab), for example,

he counted 40 stars.

121. By far the most striking discovery announced in the _Sidereal

Messenger_ was that of the bodies now known as the moons or satellites

of Jupiter. On January 7th, 1610, Galilei turned his telescope on to

Jupiter, and noticed three faint stars which caught his attention on

account of their closeness to the planet and their arrangement nearly

in a straight line with it. He looked again next night, and noticed

that they had changed their positions relatively to Jupiter, but that

the change did not seem to be such as could result from Jupiter’s own

motion, if the new bodies were fixed stars. Two nights later he was

able to confirm this conclusion, and to infer that the new bodies

were not fixed stars, but moving bodies which accompanied Jupiter in

his movements. A fourth body was noticed on January 13th, and the

motions of all four were soon recognised by Galilei as being motions of

revolution round Jupiter as a centre. With characteristic thoroughness

he watched the motions of the new bodies night after night, and by the

date of the publication of his book had already estimated with very

fair accuracy their periods of revolution round Jupiter, which ranged

between about 42 hours and 17 days; and he continued to watch their

motions for years.

[Illustration: FIG. 54.—Jupiter and its satellites as seen on Jan. 7,

1610. From the _Sidereus Nuncius_.]

The new bodies were at first called by their discoverer Medicean

planets, in honour of his patron Cosmo de Medici, the Grand Duke of

Tuscany; but it was evident that bodies revolving round a planet, as

the planets themselves revolved round the sun, formed a new class of

bodies distinct from the known planets, and the name of =satellite=,

suggested by Kepler as applicable to the new bodies as well as to the

moon, has been generally accepted.

The discovery of Jupiter’s satellites shewed the falsity of the old

doctrine that the earth was the only centre of motion; it tended,

moreover, seriously to discredit the infallibility of Aristotle and

Ptolemy, who had clearly no knowledge of the existence of such bodies;

and again those who had difficulty in believing that Venus and Mercury

could revolve round an apparently moving body, the sun, could not

but have their doubts shaken when shewn the new satellites evidently

performing a motion of just this character; and—most important

consequence of all—the very real mechanical difficulty involved in the

Coppernican conception of the moon revolving round the moving earth and

not dropping behind was at any rate shewn not to be insuperable, as

Jupiter’s satellites succeeded in performing a precisely similar feat.

The same reasons which rendered Galilei’s telescopic discoveries of

scientific importance made them also objectionable to the supporters

of the old views, and they were accordingly attacked in a number of

pamphlets, some of which are still extant and possess a certain amount

of interest. One _Martin Horky_, for example, a young German who had

studied under Kepler, published a pamphlet in which, _after_ proving to

his own satisfaction that the satellites of Jupiter did not exist, he

discussed at some length what they were, what they were like, and why

they existed. Another writer gravely argued that because the human body

had seven openings in it—the eyes, ears, nostrils, and mouth—therefore

by analogy there must be seven planets (the sun and moon being

included) and no more. However, confirmation by other observers was

soon obtained and the pendulum even began to swing in the opposite

direction, a number of new satellites of Jupiter being announced by

various observers. None of these, however, turned out to be genuine,

and Galilei’s four remained the only known satellites of Jupiter till a

few years ago (chapter XIII., § 295).

122. The reputation acquired by Galilei by the publication of the

_Messenger_ enabled him to bring to a satisfactory issue negotiations

which he had for some time been carrying on with the Tuscan court.

Though he had been well treated by the Venetians, he had begun to feel

the burden of regular teaching somewhat irksome, and was anxious to

devote more time to research and to writing. A republic could hardly

be expected to provide him with such a sinecure as he wanted, and he

accordingly accepted in the summer of 1610 an appointment as professor

at Pisa, and also as “First Philosopher and Mathematician” to the

Grand Duke of Tuscany, with a handsome salary and no definite duties

attached to either office.

123. Shortly before leaving Padua he turned his telescope on to Saturn,

and observed that the planet appeared to consist of three parts, as

shewn in the first drawing of fig. 67 (chapter VIII., § 154). On

subsequent occasions, however, he failed to see more than the central

body, and the appearances of Saturn continued to present perplexing

variations, till the mystery was solved by Huygens in 1655 (chapter

VIII., § 154).

The first discovery made at Florence (October 1610) was that Venus,

which to the naked eye appears to vary very much in brilliancy but not

in shape, was in reality at times crescent-shaped like the new moon

and passed through phases similar to some of those of the moon. This

shewed that Venus was, like the moon, a dark body in itself, deriving

its light from the sun; so that its similarity to the earth was thereby

made more evident.

[Illustration: FIG. 55.—Sun-spots. From Galilei’s _Macchie Solari_.]

124. The discovery of dark spots on the sun completed this series of

telescopic discoveries. According to his own statement Galilei first

saw them towards the end of 1610,[69] but apparently paid no particular

attention to them at the time; and, although he shewed them as a matter

of curiosity to various friends, he made no formal announcement of the

discovery till May 1612, by which time the same discovery had been

made independently by Harriot (§ 118) in England, by _John Fabricius_

(1587-? 1615) in Holland, and by the Jesuit _Christopher Scheiner_

(1575-1650) in Germany, and had been published by Fabricius (June

1611). As a matter of fact dark spots had been seen with the naked

eye long before, but had been generally supposed to be caused by the

passage of Mercury in front of the sun. The presence on the sun of such

blemishes as black spots, the “mutability” involved in their changes in

form and position, and their formation and subsequent disappearance,

were all distasteful to the supporters of the old views, according

to which celestial bodies were perfect and unchangeable. The fact,

noticed by all the early observers, that the spots appeared to move

across the face of the sun from the eastern to the western side (_i.e._

roughly from left to right, as seen at midday by an observer in our

latitudes), gave at first sight countenance to the view, championed by

Scheiner among others, that the spots might really be small planets

revolving round the sun, and appearing as dark objects whenever they

passed between the sun and the observer. In three letters to his friend

Welser, a merchant prince of Augsburg, written in 1612 and published

in the following year,[70] Galilei, while giving a full account of his

observations, gave a crushing refutation of this view; proved that

the spots must be on or close to the surface of the sun, and that the

motions observed were exactly such as would result if the spots were

attached to the sun, and it revolved on an axis in a period of about a

month; and further, while disclaiming any wish to speak confidently,

called attention to several of their points of resemblance to clouds.

One of his arguments against Scheiner’s views is so simple and at the

same time so convincing, that it may be worth while to reproduce it as

an illustration of Galilei’s method, though the controversy itself is

quite dead.

Galilei noticed, namely, that while a spot took about fourteen days

to cross from one side of the sun to the other, and this time was the

same whether the spot passed through the centre of the sun’s disc, or

along a shorter path at some distance from it, its rate of motion was

by no means uniform, but that the spot’s motion always appeared much

slower when near the edge of the sun than when near the centre. This he

recognised as an effect of foreshortening, which would result if, and

only if, the spot were near the sun.

If, for example, in the figure, the circle represent a section of

the sun by a plane through the observer at O, and A, B, C, D, E be

points taken at equal distances along the surface of the sun, so as

to represent the positions of an object on the sun at equal intervals

of time, on the assumption that the sun revolves uniformly, then the

apparent motion from A to B, as seen by the observer at O, is measured

by the angle A O B, and is obviously much less than that from D to E,

measured by the angle D O E, and consequently an object attached to

the sun must appear to move more slowly from A to B, _i.e._ near the

sun’s edge, than from D to E, near the centre. On the other hand, if

the spot be a body revolving round the sun at some distance from it,

_e.g._ along the dotted circle _c d e_, then if _c_, _d_, _e_ be taken

at equal distances from one another, the apparent motion from _c_ to

_d_, measured again by the angle _c_ O _d_, is only very slightly less

than that from _d_ to _e_, measured by the angle _d_ O _e_. Moreover,

it required only a simple calculation, performed by Galilei in several

cases, to express these results in a numerical shape, and so to infer

from the actual observations that the spots could not be more than

a very moderate distance from the sun. The only escape from this

conclusion was by the assumption that the spots, if they were bodies

revolving round the sun, moved irregularly, in such a way as always to

be moving fastest when they happened to be between the centre of the

sun and the earth, whatever the earth’s position might be at the time,

a procedure for which, on the one hand, no sort of reason could be

given, and which, on the other, was entirely out of harmony with the

uniformity to which mediæval astronomy clung so firmly.

[Illustration: FIG. 56.—Galilei’s proof that sun-spots are not planets.]

The rotation of the sun about an axis, thus established, might

evidently have been used as an argument in support of the view that

the earth also had such a motion, but, as far as I am aware, neither

Galilei nor any contemporary noticed the analogy. Among other facts

relating to the spots observed by Galilei were the greater darkness

of the central parts, some of his drawings (see fig. 55) shewing, like

most modern drawings, a fairly well-marked line of division between

the central part (or =umbra=) and the less dark fringe (or =penumbra=)

surrounding it; he noticed also that spots frequently appeared in

groups, that the members of a group changed their positions relatively

to one another, that individual spots changed their size and shape

considerably during their lifetime, and that spots were usually

most plentiful in two regions on each side of the sun’s equator,

corresponding roughly to the tropics on our own globe, and were never

seen far beyond these limits.

Similar observations were made by other telescopists, and to Scheiner

belongs the credit of fixing, with considerably more accuracy than

Galilei, the position of the sun’s axis and equator and the time of its

rotation.

125. The controversy with Scheiner as to the nature of spots

unfortunately developed into a personal quarrel as to their respective

claims to the discovery of spots, a controversy which made Scheiner his

bitter enemy, and probably contributed not a little to the hostility

with which Galilei was henceforward regarded by the Jesuits. Galilei’s

uncompromising championship of the new scientific ideas, the slight

respect which he shewed for established and traditional authority, and

the biting sarcasms with which he was in the habit of greeting his

opponents, had won for him a large number of enemies in scientific

and philosophic circles, particularly among the large party who spoke

in the name of Aristotle, although, as Galilei was never tired of

reminding them, their methods of thought and their conclusions would in

all probability have been rejected by the great Greek philosopher if he

had been alive.

It was probably in part owing to his consciousness of a growing

hostility to his views, both in scientific and in ecclesiastical

circles, that Galilei paid a short visit to Rome in 1611, when he

met with a most honourable reception and was treated with great

friendliness by several cardinals and other persons in high places.

Unfortunately he soon began to be drawn into a controversy as to the

relative validity in scientific matters of observation and reasoning

on the one hand, and of the authority of the Church and the Bible on

the other, a controversy which began to take shape about this time and

which, though its battle-field has shifted from science to science, has

lasted almost without interruption till modern times.

In 1611 was published a tract maintaining Jupiter’s satellites to

be unscriptural. In 1612 Galilei consulted Cardinal Conti as to the

astronomical teaching of the Bible, and obtained from him the opinion

that the Bible appeared to discountenance both the Aristotelian

doctrine of the immutability of the heavens and the Coppernican

doctrine of the motion of the earth. A tract of Galilei’s on floating

bodies, published in 1612, roused fresh opposition, but on the other

hand Cardinal Barberini (who afterwards, as Urban VIII., took a leading

part in his persecution) specially thanked him for a presentation

copy of the book on sun-spots, in which Galilei, for the first time,

clearly proclaimed in public his adherence to the Coppernican system.

In the same year (1613) his friend and follower, Father Castelli, was

appointed professor of mathematics at Pisa, with special instructions

not to lecture on the motion of the earth. Within a few months Castelli

was drawn into a discussion on the relations of the Bible to astronomy,

at the house of the Grand Duchess, and quoted Galilei in support of his

views; this caused Galilei to express his opinions at some length in a

letter to Castelli, which was circulated in manuscript at the court.

To this a Dominican preacher, Caccini, replied a few months afterwards

by a violent sermon on the text, “Ye Galileans, why stand ye gazing

up into heaven?”[71] and in 1615 Galilei was secretly denounced to

the Inquisition on the strength of the letter to Castelli and other

evidence. In the same year he expanded the letter to Castelli into a

more elaborate treatise, in the form of a _Letter to the Grand Duchess

Christine_, which was circulated in manuscript, but not printed till

1636. The discussion of the bearing of particular passages of the

Bible (_e.g._ the account of the miracle of Joshua) on the Ptolemaic

and Coppernican systems has now lost most of its interest; it may,

however, be worth noticing that on the more general question Galilei

quotes with approval the saying of Cardinal Baronius, “That the

intention of the Holy Ghost is to teach us not how the heavens go, but

how to go to heaven,”[72] and the following passage gives a good idea

of the general tenor of his argument:—

“Methinks, that in the Discussion of Natural Problemes we ought not

to begin at the authority of places of Scripture; but at Sensible

Experiments and Necessary Demonstrations. For ... Nature being

inexorable and immutable, and never passing the bounds of the Laws

assigned her, as one that nothing careth, whether her abstruse reasons

and methods of operating be or be not exposed to the capacity of men;

I conceive that that concerning Natural Effects, which either sensible

experience sets before our eyes, or Necessary Demonstrations do prove

unto us, ought not, upon any account, to be called into question, much

less condemned upon the testimony of Texts of Scripture, which may

under their words, couch senses seemingly contrary thereto.”[73]

126. Meanwhile his enemies had become so active that Galilei thought

it well to go to Rome at the end of 1615 to defend his cause. Early

in the next year a body of theologians known as the Qualifiers of the

Holy Office (Inquisition), who had been instructed to examine certain

Coppernican doctrines, reported:—

“That the doctrine that the sun was the centre of the world and

immoveable was false and absurd, formally heretical and contrary

to Scripture, whereas the doctrine that the earth was not the

centre of the world but moved, and has further a daily motion, was

philosophically false and absurd and theologically at least erroneous.”

In consequence of this report it was decided to censure Galilei, and

the Pope accordingly instructed Cardinal Bellarmine “to summon Galilei

and admonish him to abandon the said opinion,” which the Cardinal

did.[74] Immediately afterwards a decree was issued condemning the

opinions in question and placing on the well-known _Index of Prohibited

Books_ three books containing Coppernican views, of which the _De

Revolutionibus_ of Coppernicus and another were only suspended “until

they should be corrected,” while the third was altogether prohibited.

The necessary corrections to the _De Revolutionibus_ were officially

published in 1620, and consisted only of a few alterations which

tended to make the essential principles; of the book appear as mere

mathematical hypotheses, convenient for calculation. Galilei seems to

have been on the whole well satisfied with the issue of the inquiry, as

far as he was personally concerned, and after obtaining from Cardinal

Bellarmine a certificate that he had neither abjured his opinions nor

done penance for them, stayed on in Rome for some months to shew that

he was in good repute there.

127. During the next few years Galilei, who was now more than fifty,

suffered a good deal from ill-health and was comparatively inactive.

He carried on, however, a correspondence with the Spanish court on

a method of ascertaining the longitude at sea by means of Jupiter’s

satellites. The essential problem in finding the longitude is to obtain

the time as given by the sun at the required place and also that at

some place the longitude of which is known. If, for example, midday at

Rome occurs an hour earlier than in London, the sun takes an hour to

travel from the meridian of Rome to that of London, and the longitude

of Rome is 15° east of that of London. At sea it is easy to ascertain

the local time, _e.g._ by observing when the sun is highest in the sky,

but the great difficulty, felt in Galilei’s time and long afterwards

(chapter X., §§ 197, 226), was that of ascertaining the time at some

standard place. Clocks were then, and long afterwards, not to be relied

upon to keep time accurately during a long ocean voyage, and some

astronomical means of determining the time was accordingly wanted.

Galilei’s idea was that if the movements of Jupiter’s satellites, and

in particular the eclipses which constantly occurred when a satellite

passed into Jupiter’s shadow, could be predicted, then a table could be

prepared giving the times, according to some standard place, say Rome,

at which the eclipses would occur, and a sailor by observing the local

time of an eclipse and comparing it with the time given in the table

could ascertain by how much his longitude differed from that of Rome.

It is, however, doubtful whether the movements of Jupiter’s satellites

could at that time be predicted accurately enough to make the method

practically useful, and in any case the negotiations came to nothing.

In 1618 three comets appeared, and Galilei was soon drawn into a

controversy on the subject with a Jesuit of the name of Grassi. The

controversy was marked by the personal bitterness which was customary,

and soon developed so as to include larger questions of philosophy and

astronomy. Galilei’s final contribution to it was published in 1623

under the title _Il Saggiatore_ (The Assayer), which dealt incidentally

with the Coppernican theory, though only in the indirect way which the

edict of 1616 rendered necessary. In a characteristic passage, for

example, Galilei says:—

“Since the motion attributed to the earth, which I, as a pious and

Catholic person, consider most false, and not to exist, accommodates

itself so well to explain so many and such different phenomena, I

shall not feel sure ... that, false as it is, it may not just as

deludingly correspond with the phenomena of comets”;

and again, in speaking of the rival systems of Coppernicus and Tycho,

he says:—

“Then as to the Copernican hypothesis, if by the good fortune of

us Catholics we had not been freed from error and our blindness

illuminated by the Highest Wisdom, I do not believe that such grace

and good fortune could have been obtained by means of the reasons and

observations given by Tycho.”

Although in scientific importance the _Saggiatore_ ranks far below

many others of Galilei’s writings, it had a great reputation as a

piece of brilliant controversial writing, and notwithstanding its

thinly veiled Coppernicanism, the new Pope, Urban VIII., to whom it

was dedicated, was so much pleased with it that he had it read aloud

to him at meals. The book must, however, have strengthened the hands

of Galilei’s enemies, and it was probably with a view to counteracting

their influence that he went to Rome next year, to pay his respects

to Urban and congratulate him on his recent elevation. The visit was

in almost every way a success; Urban granted to him several friendly

interviews, promised a pension for his son, gave him several presents,

and finally dismissed him with a letter of special recommendation to

the new Grand Duke of Tuscany, who had shewn some signs of being less

friendly to Galilei than his father. On the other hand, however, the

Pope refused to listen to Galilei’s request that the decree of 1616

should be withdrawn.

128. Galilei now set seriously to work on the great astronomical

treatise, the _Dialogue on the Two Chief Systems of the World, the

Ptolemaic and Coppernican_, which he had had in mind as long ago as

1610, and in which he proposed to embody most of his astronomical work

and to collect all the available evidence bearing on the Coppernican

controversy. The form of a dialogue was chosen, partly for literary

reasons, and still more because it enabled him to present the

Coppernican case as strongly as he wished through the mouths of some

of the speakers, without necessarily identifying his own opinions

with theirs. The manuscript was almost completed in 1629, and in the

following year Galilei went to Rome to obtain the necessary licence

for printing it. The censor had some alterations made and then gave

the desired permission for printing at Rome, on condition that the

book was submitted to him again before being finally printed off. Soon

after Galilei’s return to Florence the plague broke out, and quarantine

difficulties rendered it almost necessary that the book should be

printed at Florence instead of at Rome. This required a fresh licence,

and the difficulty experienced in obtaining it shewed that the Roman

censor was getting more and more doubtful about the book. Ultimately,

however, the introduction and conclusion having been sent to Rome for

approval and probably to some extent rewritten there, and the whole

work having been approved by the Florentine censor, the book was

printed and the first copies were ready early in 1632, bearing both the

Roman and the Florentine _imprimatur_.

129. The Dialogue extends over four successive days, and is carried on

by three speakers, of whom Salviati is a Coppernican and Simplicio an

Aristotelian philosopher, while Sagredo is avowedly neutral, but on

almost every occasion either agrees with Salviati at once or is easily

convinced by him, and frequently joins in casting ridicule upon the

arguments of the unfortunate Simplicio. Though many of the arguments

have now lost their immediate interest, and the book is unduly long,

it is still very readable, and the specimens of scholastic reasoning

put into the mouth of Simplicio and the refutation of them by the other

speakers strike the modern reader as excellent fooling.

Many of the arguments used had been published by Galilei in earlier

books, but gain impressiveness and cogency by being collected and

systematically arranged. The Aristotelian dogma of the immutability

of the celestial bodies is once more belaboured, and shewn to be not

only inconsistent with observations of the moon, the sun, comets, and

new stars, but to be in reality incapable of being stated in a form

free from obscurity and self-contradiction. The evidence in favour of

the earth’s motion derived from the existence of Jupiter’s satellites

and from the undoubted phases of Venus, from the suspected phases of

Mercury and from the variations in the apparent size of Mars, are once

more insisted on. The greater simplicity of the Coppernican explanation

of the daily motion of the celestial sphere and of the motion of the

planets is forcibly urged and illustrated in detail. It is pointed

out that on the Coppernican hypothesis all motions of revolution or

rotation take place in the same direction (from west to east), whereas

the Ptolemaic hypothesis requires some to be in one direction, some

in another. Moreover the apparent daily motion of the stars, which

appears simple enough if the stars are regarded as rigidly attached

to a material sphere, is shewn in a quite different aspect if, as

even Simplicio admits, no such sphere exists, and each star moves in

some sense independently. A star near the pole must then be supposed

to move far more slowly than one near the equator, since it describes

a much smaller circle in the same time; and further—an argument very

characteristic of Galilei’s ingenuity in drawing conclusions from

known facts—owing to the precession of the equinoxes (chapter II., §

42, and IV., § 84) and the consequent change of the position of the

pole among the stars, some of those stars which in Ptolemy’s time

were describing very small circles, and therefore moving slowly, must

now be describing large ones at a greater speed, and _vice versa_. An

extremely complicated adjustment of motions becomes therefore necessary

to account for observations which Coppernicus explained adequately by

the rotation of the earth and a simple displacement of its axis of

rotation.

Salviati deals also with the standing difficulty that the annual

motion of the earth ought to cause a corresponding apparent motion

of the stars, and that if the stars be assumed so far off that this

motion is imperceptible, then some of the stars themselves must be at

least as large as the earth’s orbit round the sun. Salviati points out

that the apparent or angular magnitudes of the fixed stars, avowedly

difficult to determine, are in reality almost entirely illusory, being

due in great part to an optical effect known as =irradiation=, in

virtue of which a bright object always tends to appear enlarged;[75]

and that there is in consequence no reason to suppose the stars nearly

as large as they might otherwise be thought to be. It is suggested

also that the most promising way of detecting the annual motion of

stars resulting from the motion of the earth would be by observing

the relative displacement of two stars close together in the sky (and

therefore nearly in the same direction), of which one might be presumed

from its greater brightness to be nearer than the other. It is, for

example, evident that if, in the figure, E, E′ represent two positions

of the earth in its path round the sun, and A, B two stars at different

distances, but nearly in the same direction, then to the observer at

E the star A appears to the left of B, whereas six months afterwards,

when the observer is at E′, A appears to the right of B. Such a motion

of one star with respect to another close to it would be much more

easily observed than an alteration of the same amount in the distance

of the star from some standard point such as the pole. Salviati points

out that accurate observations of this kind had not been made, and that

the telescope might be of assistance for the purpose. This method,

known as the =double-star= or =differential method of parallax=, was in

fact the first to lead—two centuries later—to a successful detection of

the motion in question (chapter XIII., § 278).

[Illustration: FIG. 57.—The differential method of parallax.]

130. Entirely new ground is broken in the _Dialogue_ when Galilei’s

discoveries of the laws of motion of bodies are applied to the problem

of the earth’s motion. His great discovery, which threw an entirely new

light on the mechanics of the solar system, was substantially the law

afterwards given by Newton as the first of his three laws of motion,

in the form: _Every body continues in its state of rest or of uniform

motion in a straight line, except in so far as it is compelled by force

applied to it to change that state._ Putting aside for the present

any discussion of _force_, a conception first made really definite by

Newton, and only imperfectly grasped by Galilei, we may interpret this

law as meaning that a body has no more inherent tendency to diminish

its motion or to stop than it has to increase its motion or to start,

and that any alteration in either the speed or the direction of a

body’s motion is to be explained by the action on it of some other

body, or at any rate by some other assignable cause. Thus a stone

thrown along a road comes to rest on account of the friction between

it and the ground, a ball thrown up into the air ascends more and more

slowly and then falls to the ground on account of that attraction

of the earth on it which we call its weight. As it is impossible to

entirely isolate a body from all others, we cannot experimentally

realise the state of things in which a body goes on moving indefinitely

in the same direction and at the same rate; it may, however, be shewn

that the more we remove a body from the influence of others, the less

alteration is there in its motion. The law is therefore, like most

scientific laws, an abstraction referring to a state of things to

which we may approximate in nature. Galilei introduces the idea in the

Dialogue by means of a ball on a smooth inclined plane. If the ball

is projected upwards, its motion is gradually retarded; if downwards,

it is continually accelerated. This is true if the plane is fairly

smooth—like a well-planed plank—and the inclination of the plane not

very small. If we imagine the experiment performed on an ideal plane,

which is supposed _perfectly_ smooth, we should expect the same results

to follow, however small the inclination of the plane. Consequently,

if the plane were quite level, so that there is no distinction between

up and down, we should expect the motion to be neither retarded nor

accelerated, but to continue without alteration. Other more familiar

examples are also given of the tendency of a body, when once in

motion, to continue in motion, as in the case of a rider whose horse

suddenly stops, or of bodies in the cabin of a moving ship which have

no tendency to lose the motion imparted to them by the ship, so that,

_e.g._, a body falls down to all appearances exactly as if the rest

of the cabin were at rest, and therefore, in reality, while falling

retains the forward motion which it shares with the ship and its

contents. Salviati states also that—contrary to general belief—a stone

dropped from the masthead of a ship in motion falls at the foot of the

mast, not behind it, but there is no reference to the experiment having

been actually performed.

This mechanical principle being once established, it becomes easy to

deal with several common objections to the supposed motion of the

earth. The case of a stone dropped from the top of a tower, which if

the earth be in reality moving rapidly from west to east might be

expected to fall to the west in its descent, is easily shewn to be

exactly parallel to the case of a stone dropped from the masthead of

a ship in motion. The motion towards the east, which the stone when

resting on the tower shares with the tower and the earth, is not

destroyed in its descent, and it is therefore entirely in accordance

with the Coppernican theory that the stone should fall as it does at

the foot of the tower.[76] Similarly, the fact that the clouds, the

atmosphere in general, birds flying in it, and loose objects on the

surface of the earth, shew no tendency to be left behind as the earth

moves rapidly eastward, but are apparently unaffected by the motion of

the earth, is shewn to be exactly parallel to the fact that the flies

in a ship’s cabin and the loose objects there are in no way affected

by the uniform onward motion of the ship (though the irregular motions

of pitching and rolling do affect them). The stock objection that

a cannon-ball shot westward should, on the Coppernican hypothesis,

carry farther than one shot eastward under like conditions, is met

in the same way; but it is further pointed out that, owing to the

imperfection of gunnery practice, the experiment could not really be

tried accurately enough to yield any decisive result.

The most unsatisfactory part of the _Dialogue_ is the fourth day’s

discussion, on the tides, of which Galilei suggests with great

confidence an explanation based merely on the motion of the earth,

while rejecting with scorn the suggestion of Kepler and others—correct

as far as it went—that they were caused by some influence emanating

from the moon. It is hardly to be wondered at that the rudimentary

mechanical and mathematical knowledge at Galilei’s command should not

have enabled him to deal correctly with a problem of which the vastly

more powerful resources of modern science can only give an imperfect

solution (cf. chapter XI., § 248, and chapter XIII., § 292).

131. The book as a whole was in effect, though not in form, a

powerful—indeed unanswerable—plea for Coppernicanism. Galilei tried to

safeguard his position, partly by the use of dialogue, and partly by

the very remarkable introduction, which was not only read and approved

by the licensing authorities, but was in all probability in part the

composition of the Roman censor and of the Pope. It reads to us like

a piece of elaborate and thinly veiled irony, and it throws a curious

light on the intelligence or on the seriousness of the Pope and the

censor, that they should have thus approved it:—

“Judicious reader, there was published some years since in _Rome_ a

salutiferous Edict, that, for the obviating of the dangerous Scandals

of the present Age, imposed a reasonable Silence upon the Pythagorean

Opinion of the Mobility of the Earth. There want not such as

unadvisedly affirm, that the Decree was not the production of a sober

Scrutiny, but of an informed passion; and one may hear some mutter

that Consultors altogether ignorant of Astronomical observations ought

not to clipp the wings of speculative wits with rash prohibitions. My

zeale cannot keep silence when I hear these inconsiderate complaints.

I thought fit, as being thoroughly acquainted with that prudent

Determination, to appear openly upon the Theatre of the World as a

Witness of the naked Truth. I was at that time in _Rome_, and had

not only the audiences, but applauds of the most Eminent Prelates of

that Court; nor was that Decree published without Previous Notice

given me thereof. Therefore it is my resolution in the present case

to give Foreign Nations to see, that this point is as well understood

in _Italy_, and particularly in _Rome_, as Transalpine Diligence can

imagine it to be: and collecting together all the proper speculations

that concerne the _Copernican Systeme_ to let them know, that the

notice of all preceded the Censure of the _Roman Court_; and that

there proceed from this Climate not only Doctrines for the health of

the Soul, but also ingenious Discoveries for the recreating of the

Mind.... I hope that by these considerations the world will know, that

if other Nations have Navigated more than we, we have not studied less

than they; and that our returning to assert the Earth’s stability, and

to take the contrary only for a Mathematical _Capriccio_, proceeds

not from inadvertency of what others have thought thereof, but (had

one no other inducements), from these reasons that Piety, Religion,

the Knowledge of the Divine Omnipotency, and a consciousness of the

incapacity of man’s understanding dictate unto us.”[77]

132. Naturally Galilei’s many enemies were not long in penetrating

these thin disguises, and the immense success of the book only

intensified the opposition which it excited; the Pope appears to have

been persuaded that Simplicio—the butt of the whole dialogue—was

intended for himself, a supposed insult which bitterly wounded his

vanity; and it was soon evident that the publication of the book

could not be allowed to pass without notice. In June 1632 a special

commission was appointed to inquire into the matter—an unusual

procedure, probably meant as a mark of consideration for Galilei—and

two months later the further issue of copies of the book was

prohibited, and in September a papal mandate was issued requiring

Galilei to appear personally before the Inquisition. He was evidently

frightened by the summons, and tried to avoid compliance through

the good offices of the Tuscan court and by pleading his age and

infirmities, but after considerable delay, at the end of which the

Pope issued instructions to bring him if necessary by force and in

chains, he had to submit, and set off for Rome early in 1633. Here

he was treated with unusual consideration, for whereas in general

even the most eminent offenders under trial by the Inquisition were

confined in its prisons, he was allowed to live with his friend

Niccolini, the Tuscan ambassador, throughout the trial, with the

exception of a period of about three weeks, which he spent within the

buildings of the Inquisition, in comfortable rooms belonging to one

of the officials, with permission to correspond with his friends,

to take exercise in the garden, and other privileges. At his first

hearing before the Inquisition, his reply to the charge of having

violated the decree of 1616 (§ 126) was that he had not understood

that the decree or the admonition given to him forbade the teaching

of the Coppernican theory as a mere “hypothesis,” and that his book

had not upheld the doctrine in any other way. Between his first and

second hearing the Commission, which had been examining his book,

reported that it did distinctly defend and maintain the obnoxious

doctrines, and Galilei, having been meanwhile privately advised by

the Commissary-General of the Inquisition to adopt a more submissive

attitude, admitted at the next hearing that on reading his book again

he recognised that parts of it gave the arguments for Coppernicanism

more strongly than he had at first thought. The pitiable state to which

he had been reduced was shewn by the offer which he now made to write

a continuation to the Dialogue which should as far as possible refute

his own Coppernican arguments. At the final hearing on June 21st he

was examined under threat of torture,[78] and on the next day he was

brought up for sentence. He was convicted “of believing and holding the

doctrines—false and contrary to the Holy and Divine Scriptures—that the

sun is the centre of the world, and that it does not move from east

to west, and that the earth does move and is not the centre of the

world; also that an opinion can be held and supported as probable after

it has been declared and decreed contrary to the Holy Scriptures.”

In punishment, he was required to “abjure, curse, and detest the

aforesaid errors,” the abjuration being at once read by him on his

knees; and was further condemned to the “formal prison of the Holy

Office” during the pleasure of his judges, and required to repeat the

seven penitential psalms once a week for three years. On the following

day the Pope changed the sentence of imprisonment into confinement at

a country-house near Rome belonging to the Grand Duke, and Galilei

moved there on June 24th.[79] On petitioning to be allowed to return

to Florence, he was at first allowed to go as far as Siena, and at the

end of the year was permitted to retire to his country-house at Arcetri

near Florence, on condition of not leaving it for the future without

permission, while his intercourse with scientific and other friends was

jealously watched.

[Illustration: GALILEI.]

The story of the trial reflects little credit either on Galilei or

on his persecutors. For the latter, it may be urged that they acted

with unusual leniency considering the customs of the time; and it

is probable that many of those who were concerned in the trial were

anxious to do as little injury to Galilei as possible, but were

practically forced by the party personally hostile to him to take some

notice of the obvious violation of the decree of 1616. It is easy to

condemn Galilei for cowardice, but it must be borne in mind, on the

one hand, that he was at the time nearly seventy, and much shaken

in health, and, on the other, that the Roman Inquisition, if not as

cruel as the Spanish, was a very real power in the early 17th century;

during Galilei’s lifetime (1600) Giordano Bruno had been burnt alive

at Rome for writings which, in addition to containing religious and

political heresies, supported the Coppernican astronomy and opposed

the traditional Aristotelian philosophy. Moreover, it would be unfair

to regard his submission as due merely to considerations of personal

safety, for—apart from the question whether his beloved science would

have gained anything by his death or permanent imprisonment—there

can be no doubt that Galilei was a perfectly sincere member of his

Church, and although he did his best to convince individual officers

of the Church of the correctness of his views, and to minimise the

condemnation of them passed in 1616, yet he was probably prepared,

when he found that the condemnation was seriously meant by the Pope,

the Holy Office, and others, to believe that in some senses at least

his views must be wrong, although, as a matter of observation and pure

reason, he was unable to see how or why. In fact, like many other

excellent people, he kept watertight compartments in his mind, respect

for the Church being in one and scientific investigation in another.

Copies of the sentence on Galilei and of his abjuration were at once

circulated in Italy and in Roman Catholic circles elsewhere, and a

decree of the Congregation of the Index was also issued adding the

_Dialogue_ to the three Coppernican books condemned in 1616, and to

Kepler’s _Epitome_ of the Coppernican Astronomy (chapter VII., §

145), which had been put on the _Index_ shortly afterwards. It may

be of interest to note that these five books still remained in the

edition of the _Index of Prohibited Books_ which was issued in 1819

(with appendices dated as late as 1821), but disappeared from the next

edition, that of 1835.

133. The rest of Galilei’s life may be described very briefly. With

the exception of a few months, during which he was allowed to be at

Florence for the sake of medical treatment, he remained continuously

at Arcetri, evidently pretty closely watched by the agents of the

Holy Office, much restricted in his intercourse with his friends, and

prevented from carrying on his studies in the directions which he liked

best. He was moreover very infirm, and he was afflicted by domestic

troubles, especially by the death in 1634 of his favourite child, a nun

in a neighbouring convent. But his spirit was not broken, and he went

on with several important pieces of work, which he had begun earlier

in his career. He carried a little further the study of his beloved

Medicean Planets and of the method of finding longitude based on

their movements (§ 127), and negotiated on the subject with the Dutch

government. He made also a further discovery relating to the moon, of

sufficient importance to deserve a few words of explanation.

[Illustration: FIG. 58.—The daily libration of the moon.]

It had long been well known that as the moon describes her monthly path

round the earth we see the same markings substantially in the same

positions on the disc, so that substantially the same face of the moon

is turned towards the earth. It occurred to Galilei to inquire whether

this was accurately the case, or whether, on the contrary, some change

in the moon’s disc could be observed. He saw that if, as seemed likely,

the line joining the centres of the earth and moon always passed

through the same point on the moon’s surface, nevertheless certain

alterations in an observer’s position on the earth would enable him to

see different portions of the moon’s surface from time to time. The

simplest of these alterations is due to the daily motion of the earth.

Let us suppose for simplicity that the observer is on the earth’s

equator, and that the moon is at the time in the celestial equator. Let

the larger circle in fig. 58 represent the earth’s equator, and the

smaller circle the section of the moon by the plane of the equator.

Then in about 12 hours the earth’s rotation carries the observer from

A, where he sees the moon rising, to B, where he sees it setting. When

he is at C, on the line joining the centres of the earth and moon, the

point O appears to be in the centre of the moon’s disc, and the portion

_c_ O _c′_ is visible, _c_ R _c′_ invisible. But when the observer is

at A, the point P, on the right of O, appears in the centre, and the

portion _a_ P _a′_ is visible, so that _c′ a′_ is now visible and _a

c_ invisible. In the same way, when the observer is at B, he can see

the portion _c b_, while _b′ c′_ is invisible and Q appears to be in

the centre of the disc. Thus in the course of the day the portion _a_ O

_b′_ (dotted in the figure) is constantly visible and _b_ R _a′_ (also

dotted) constantly invisible, while _a c b_ and _a′ c′ b′_ alternately

come into view and disappear. In other words, when the moon is rising

we see a little more of the side which is the then uppermost, and

when she is setting we see a little more of the other side which is

uppermost in this position. A similar explanation applies when the

observer is not on the earth’s equator, but the geometry is slightly

more complicated. In the same way, as the moon passes from south to

north of the equator and back as she revolves round the earth, we see

alternately more and less of the northern and southern half of the

moon. This set of changes—the simplest of several somewhat similar ones

which are now known as =librations= of the moon—being thus thought of

as likely to occur, Galilei set to work to test their existence by

observing certain markings of the moon usually visible near the edge,

and at once detected alterations in their distance from the edge, which

were in general accordance with his theoretical anticipations. A more

precise inquiry was however interrupted by failing sight, culminating

(at the end of 1636) in total blindness.

But the most important work of these years was the completion of the

great book, in which he summed up and completed his discoveries in

mechanics, _Mathematical Discourses and Demonstrations concerning

Two New Sciences, relating to Mechanics and to Local Motion_. It was

written in the form of a dialogue between the same three speakers who

figured in the Dialogue on the Systems, but is distinctly inferior in

literary merit to the earlier work. We have here no concern with a

large part of the book, which deals with the conditions under which

bodies are kept, at rest by forces applied to them (statics), and

certain problems relating to the resistance of bodies to fracture and

to bending, though in both of these subjects Galilei broke new ground.

More important astronomically—and probably intrinsically also—is what

he calls the science of local motion,[80] which deals with the motion

of bodies. He builds up on the basis of his early experiments (§

116) a theory of falling bodies, in which occurs for the first time

the important idea of =uniformly accelerated motion=, or =uniform

acceleration=, _i.e._ motion in which the moving body receives in every

equal interval of time an equal increase of velocity. He shews that

the motion of a falling body is—except in so far as it is disturbed

by the air—of this nature, and that, as already stated, the motion

is the same for all bodies, although his numerical estimate is not

at all accurate.[81] From this fundamental law he works out a number

of mathematical deductions, connecting the space fallen through, the

velocity, and the time elapsed, both for the case of a body falling

freely and for one falling down an inclined plane. He gives also a

correct elementary theory of projectiles, in the course of which he

enunciates more completely than before the law of inertia already

referred to (§ 130), although Galilei’s form is still much less general

than Newton’s:—

_Conceive a body projected or thrown along a horizontal plane, all

impediments being removed. Now it is clear by what we have said before

at length that its motion will be uniform and perpetual along the said

plane, if the plane extend indefinitely._

In connection with projectiles, Galilei also appears to realise that

a body may be conceived as having motions in two different directions

simultaneously, and that each may be treated as independent of the

other, so that, for example, if a bullet is shot horizontally out of

a gun, its downward motion, due to its weight, is unaffected by its

horizontal motion, and consequently it reaches the ground at the same

time as a bullet simply allowed to drop; but Galilei gives no general

statement of this principle, which was afterwards embodied by Newton in

his Second Law of Motion.

The treatise on the _Two New Sciences_ was finished in 1636, and, since

no book of Galilei’s could be printed in Italy, it was published after

some little delay at Leyden in 1638. In the same year his eyesight,

which he had to some extent recovered after his first attack of

blindness, failed completely, and four years later (January 8th, 1642)

the end came.

134. Galilei’s chief scientific discoveries have already been noticed.

The telescopic discoveries, on which much of his popular reputation

rests, have probably attracted more than their fair share of attention;

many of them were made almost simultaneously by others, and the rest,

being almost inevitable results of the invention of the telescope,

could not have been delayed long. But the skilful use which Galilei

made of them as arguments for the Coppernican system, the no less

important support which his dynamical discoveries gave to the same

cause, the lucidity and dialectic brilliance with which he marshalled

the arguments in favour of his views and demolished those of his

opponents, together with the sensational incidents of his persecution,

formed conjointly a contribution to the Coppernican controversy which

was in effect decisive. Astronomical textbooks still continued to give

side by side accounts of the Ptolemaic and of the Coppernican systems,

and the authors, at any rate if they were good Roman Catholics, usually

expressed, in some more or less perfunctory way, their adherence

to the former, but there was no real life left in the traditional

astronomy; new advances in astronomical theory were all on Coppernican

lines, and in the extensive scientific correspondence of Newton and

his contemporaries the truth of the Coppernican system scarcely ever

appears as a subject for discussion.

Galilei’s dynamical discoveries, which are only in part of astronomical

importance, are in many respects his most remarkable contribution to

science. For whereas in astronomy he was building on foundations laid

by previous generations, in dynamics it was no question of improving

or developing an existing science, but of creating a new one. From his

predecessors he inherited nothing but erroneous traditions and obscure

ideas; and when these had been discarded, he had to arrive at clear

fundamental notions, to devise experiments and make observations, to

interpret his experimental results, and to follow out the mathematical

consequences of the simple laws first arrived at. The positive results

obtained may not appear numerous, if viewed from the standpoint of our

modern knowledge, but they sufficed to constitute a secure basis for

the superstructure which later investigators added.

It is customary to associate with our countryman Francis Bacon

(1561-1627) the reform in methods of scientific discovery which

took place during the seventeenth century, and to which much of the

rapid progress in the natural sciences made since that time must be

attributed. The value of Bacon’s theory of scientific discovery is

very differently estimated by different critics, but there can be no

question of the singular ill-success which attended his attempts to

apply it in particular cases, and it may fairly be questioned whether

the scientific methods constantly referred to incidentally by Galilei,

and brilliantly exemplified by his practice, do not really contain a

large part of what is valuable in the Baconian philosophy of science,

while at the same time avoiding some of its errors. Reference has

already been made on several occasions to Galilei’s protests against

the current method of dealing with scientific questions by the

interpretation of passages in Aristotle, Ptolemy, or other writers;

and to his constant insistence on the necessity of appealing directly

to actual observation of facts. But while thus agreeing with Bacon in

these essential points, he differed from him in the recognition of

the importance, both of deducing new results from established ones by

mathematical or other processes of exact reasoning, and of using such

deductions, when compared with fresh experimental results, as a means

of verifying hypotheses provisionally adopted. This method of proof,

which lies at the base of nearly all important scientific discovery,

can hardly be described better than by Galilei’s own statement of it,

as applied to a particular case:—

“Let us therefore take this at present as a _Postulatum_, the truth

whereof we shall afterwards find established, when we shall see other

conclusions built upon this _Hypothesis_, to answer and most exactly

to agree with Experience.”[82]

A Short History of Astronomy · 第 6 / 14 章