1 Introduction

1.1 Galileo’s Theoremata

The Theoremata circa centrum gravitatis solidorum—an appendix to Discorsi e dimostrazioni matematiche intorno a due nuove scienze (Leiden 1638)—gather together Galileo’s studies on the centers of gravity of solids. Although these studies date to the years of his formation (he wrote those theorems beginning about 1587), they were printed only in 1638 after several plans to publish them fell through.

Galileo’s aim was to establish himself as a mathematician and to obtain the chair of mathematics at the University of Bologna. To this end he circulated the theorems among some noted mathematicians of his time, including Christopher Clavius, Guidobaldo dal Monte, Giuseppe Moleti, and Abraham Ortelius.Footnote 1

In these theorems Galileo determined the center of gravity of the paraboloid, the cone, and their frusta. In the Leiden version the TheoremataFootnote 2 begin with a postulate and a lemma necessary for the proofs to follow. Then for each whole solid two lemmas and two theorems are proved, and for each frustum one lemma and one theorem. The argumentative structure for all the proofs is the same: lemmas required for the proofs are proved ad hoc; in the first theorem, the positions of the centers of gravity of the inscribed and circumscribed solids are determined; in the second theorem, it is shown that the center of gravity of the solid divides the axis in a certain ratio. For the frusta, there is one theorem for each case where the ratio is found directly.

Besides the printed edition, there was previously thought to be only one other incomplete copy on these theorems. This is in the Milan, Biblioteca Ambrosiana, MS A 71 Inf., which contains on folios 95–96 only the lemma and theorem on the frustum of a cone.

Recently another incomplete witness of the Theoremata had been discovered. This is in the manuscript now in the Charles E. Young Research Library, University of California-Los Angeles with the shelfmark 170/624.

1.2 The manuscript UCLA 170/624

The manuscript was described by Neville (1986) in “The Printer’s Copy of Commandino’s Translation of Archimedes, 1558.” It is a composite codex, formerly in the Albani Library (MS 670), made of three different codicological units:

  1. 1

    the printer’s copy of Federico Commandino’s translation of Archimedes for his Archimedis Opera nonnulla (Venice, 1558) (folios 1–74);

  2. 2

    miscellaneous materials linked to Guidobaldo dal Monte,Footnote 3 partly written by himself (folios 75–91); and

  3. 3

    a text related to François Viète’s algebra (folios 92–214).Footnote 4

In recent years, several studies have examined Guidobaldo’s role not only as scientific heir to Commandino but also for the part he played in guiding the first steps of Galileo’s career and for his network of correspondents, which included Christopher Clavius in Rome and Giacomo Contarini in Venice.Footnote 5 This justifies a deeper inquiry into this second part of the manuscript, which is also related to other texts by Guidobaldo, for example the Meditatiunculae de rebus mathematicis.Footnote 6

1.3 A notebook by Guidobaldo dal Monte: the Colibeto

Muzio Oddi (1569–1639), engineer and mathematician, studied in Urbino with Guidobaldo.Footnote 7 Oddi referred on various occasions to Guidobaldo’s writings which he proved to know very well.Footnote 8 For example, in a letter dated 21 February 1635 Oddi described a text written by Guidobaldo:

A paraphrase of that passage in Hyginus on the meridian line, which I printed and I know that in his [Guidobalo’s] book that he called Colibeto there are various treatments of three, four, and more propositions together on various matters.Footnote 9

In this passage Oddi affirmed that Guidobaldo wrote a Colibeto, a booklet or folder, with problems and mathematical notes in no definite order. According to Oddi, the Colibeto contained “propositions together on diverse matters,” and in particular a discussion on the meridian line by Hyginus. Oddi also published a longer description of Guidobaldo’s account on Hyginus:

To know how to draw the meridian line on a plane to the horizon ...I wanted on this occasion to refer here to one [solution ]written by Hyginus, the ancient and famous astronomer, in the book Gromaticus ...this passage being so badly marred by the multitude of years, one can only make the construction poorly who has not seen the exposition that, at the instance of Signor Giovanni Vincenzo Pinelli of Padua, Signor Guidobaldo Marchese del Monte made for you, from whose kindness I confess to have learned all of what little knowledge I have of mathematics.Footnote 10

The text to which Oddi refers, citing Guidobaldo and his corrections to Hyginus, is found in the UCLA manuscript at folios 77–78 and \(83{-}3^{\mathrm{o}}\), which can therefore be identified as the Colibeto (or at least a part of it).Footnote 11

1.4 The purpose

In this article, our attention will focus on UCLA folios 75–76, containing Galileo’s proof of the center of gravity of the frustum of a cone, which was ultimately published among the results of Theoremata.Footnote 12

The discovery of the UCLA copy opened the possibility of giving a fuller account of Theoremata dating and development, and it can shed light on the origins of this research by the young Galileo. Moreover, it helps to explain the connections between Galileo and Guidobaldo, starting from 1587–88, in the context of Galileo’s early work. But before turning to this manuscript, it is necessary first to broaden the view by presenting the genesis of Galileo’s studies in this field and following his mathematical and academic career.

So in Sect. 2 we shall give an overview of sixteenth-century studies on centers of gravity. Then, after comparing the UCLA manuscript with other extant copies, we shall propose a dating for the composition of the Theoremata circa centrum gravitatis solidorum based on Galileo’s correspondence with the Jesuit Christopher Clavius (1538–1612) and with Guidobaldo. This dating will then be reconsidered in light of the mathematical content, which will be described in Sect. 5. We shall end with an appendix (Sect. 7) containing a description of the manuscript and an edition of the text of the lemma and theorem.

2 Centers of gravity of solids at the end of the sixteenth century

The study of centers of gravity during the sixteenth century developed as a direct consequence of the restoration of Archimedes’ corpus, and in particular of the work On the Equilibrium of Planes. This Archimedean work is in two books: the first deals with the law of the lever and the center of gravity of the triangle and the trapezium; in the second, Archimedes determined the center of gravity of a segment of a parabola and of the mixtilinear trapezium.Footnote 13 In On the Equilibrium of Planes no mention is made of the centers of gravity of solid figures, although references to this problem appeared in other Archimedean texts available to sixteenth-century mathematicians. A passage from the second book of On Floating Bodies in Commandino’s version reads:

The center of gravity of a portion of a right conoid is on the axis, which it so divides that the part that ends at the vertex is double the remaining part at the base.Footnote 14

This passage conveys the critical information that Archimedes had determined the precise location of the center of the paraboloid of revolution. The demonstration of this result was not present in any writings of Archimedes available at that time.Footnote 15

Unfortunately, the fate of On Floating Bodies was not a happy one. Although it was translated into Latin by William of Moerbeke in 1269, his translation did not become part of any of the editions of Archimedes’ works printed in the first half of the sixteenth century. The two books On Floating Bodies are absent from Luca Gaurico’s Tetragonismus id est quadratura circuli (Gaurico 1503), which contains only The Measurement of a Circle and The Quadrature of the Parabola. Tartaglia’s more complete edition (Archimedes 1543) contained only the first book of On Floating Bodies.Footnote 16

Interpretation by Commandino of the second book in his De iis quae vehuntur in aqua (Archimedes 1565a) cleared up many of the obscurities in Archimedes’ text and Moerbeke’s translation.Footnote 17

Besides the difficulties of Archimedes’ texts on centers of gravity, there was also a lack of sources. For instance, a definition of center of gravity was absent from all the works at disposal of the scholars of that period.Footnote 18 In his Liber de centro gravitatis solidorum of 1565, Commandino declared that the quaestio de centro gravitatis corporum solidorum was truly perdifficilis et perobscura.

2.1 Maurolico’s results

Francesco Maurolico (1494–1575) did not have access to Moerbeke’s translation when he devoted himself to restoring Archimedes’ theory of equilibrium and so adopted a different approach. His De momentis aequalibus libri quattuor represents a complete remaking of Archimedes’ work on the subject.Footnote 19 In the fourth book he tackled the question of finding the center of gravity of solids and in 1548 he managed to devise a brilliant demonstration for the pyramid and the regular solids, as he points out in the preface:

It now remains to treat of finding the center of gravity in solids; for this was the subject of his work that I marvel not a little was omitted by Archimedes. ...Nevertheless, the center of the pyramid could be sought out with no less labour—not to say with more—than the center of the plane triangle. So since we shall have treated in the first book the general theory of weights, in the second the centers of planes, and in the third of conic sections called parabolas, in order to understand more clearly what Archimedes wrote. Now in this fourth book we shall undertake the task.Footnote 20

Napolitani and Sutto (2001) determined that Maurolico resumed his study of the centers of gravity of solids only in 1565, extending it to the paraboloid of revolution. In that year Maurolico made a capital discovery: that the center of gravity of the paraboloid could be resolved back to that of the triangle, already known from the works of Archimedes and extensively treated by Maurolico in the second book of De momentis aequalibus.

This discovery was presented, with a not completely rigorous proof, in a manuscript (Paris, Bibliothèque Nationale, MS lat. 7466, folios 8–14) addressed to an unknown recipient, probably a Jesuit with whom Maurolico was in contact. Unfortunately, this text remained unpublished until the nineteenth century. However, the determination of the center of gravity of the paraboloid was later formalized by Maurolico and added to the fourth book of De momentis. There the proof in the manuscript was replaced by one using double contradiction, usually known as the method of exhaustion, which was closer to Archimedean rigor. Maurolico’s De momentis aequalibus libri quattuor was not printed until 1685,Footnote 21 but Maurolico’s results circulated among the mathematicians and influenced research on centers of gravity in the second half of the sixteenth century.Footnote 22

Commandino and Clavius were two of those who received Maurolico’s legacy and took up the study of centers of gravity.

2.2 Commandino’s Challenge

Federico Commandino started an in-depth study of Archimedes following a request made by the cardinal of the Vatican library Marcello Cervini who was looking for explanations concerning two works—De insidentibus aquae, William of Moerbeke’s Latin translation of Archimedes’ On floating bodies, and Ptolemy’s De analemmate—contained in a copy of Rome, Biblioteca Apostolica Vaticana, MS. Ott. lat. 1850. Cervini also asked for a corrected Latin edition thereof. Commandino began the examination of Archimedes’ texts and in 1558 he published in Venice the Archimedis opera nonnulla, a new translation of many Archimedean works, but not On Floating Bodies (Archimedes 1558).

In 1565 he completed the task entrusted to him fifteen years earlier by Cervini by printing in Bologna his edition of Moerbeke’s translation of On Floating Bodies and an original work, the Liber de centro gravitatis solidorum (Commandino 1565). In writing this text Commandino, always philologically faithful to his model, was inspired by the method of Archimedes’ On the Equilibrium of Planes.

We have evidence of a correspondence between Maurolico and Commandino on some theorems of On Conoids and Spheroids although nothing that demonstrates a direct exchange of ideas regarding centers of gravity of solids.Footnote 23

In the preface, Commandino wrote that he delayed publication after coming into possession of Maurolico’s book on centers of gravity:

But when I was in the process of writing this, the book of Francesco Maurolico of Messina was sent to me, in which that most learned and most accomplished man in these disciplines affirmed that he had written on centers of gravity of solid bodies. When I learned this, I held myself back for a time and waited silently while the work of this most renowned man, whom I always mention with honor, was brought to light.Footnote 24

The Liber de centro gravitatis solidorum starts with the definition of center of gravity and provides some results for plane figures already demonstrated by Archimedes. Commandino determined the center of gravity of simpler solids such as the prism and the cylinder; then he moved on to the more complex ones: the pyramid, cone, paraboloid and frustra (propositions XXII, XXIX and XXVI, XXXI). Commandino had thrown down the gauntlet to other mathematicians. But the challenge was not over. The theorems for frusta were not fully satisfactory: the enunciations were long and convoluted and the proofs were difficult to understand.Footnote 25 In particular, the proof for the frustum of a paraboloid was so unclear that Guidobaldo himself wrote in a letter to Galileo that it was not good, because it was not general (universale).Footnote 26 The mathematicians after Commandino took up the challenge and thus began to study the centers of gravity of solids.

2.3 From Clavius to Galileo, towards the Epilogue

Clavius should be mentioned for his indirect contribution to the development of the study of centers of gravity in the second half of the sixteenth century. He got to know Maurolico both in correspondence (from 1569) and in person during a stay in Messina in 1574.Footnote 27 On this occasion he consulted some working copies of Maurolico’s mathematical texts and brought them back to Rome, once he had returned from his travels in Sicily.Footnote 28

At the Collegio Romano Clavius established a course in higher mathematics that included centers of gravity of solids. Although he never published anything on the subject, various testimonies suggest that from the 1580s he was considered an expert.Footnote 29 The most significant comes from a letter from Guidobaldo to Galileo dated 16 January 1588, containing a reference to the theorem on the center of gravity of the frustum of a paraboloid:

Among some letters that on many days passed between Father Clavius and me, I wrote him that the last [proposition] of Commandino’s De centro gravitatis solidorum was not sound because it was not general; he sent me then his own proof, very different from yours.Footnote 30

Traces of Clavius’s proof remain today among Guidobaldo’s papers in the Meditatiunculae de rebus mathematicis.Footnote 31 Clavius’s demonstration, transcribed by Guidobaldo, follows Commandino’s deductive pattern, but with even greater attention to detail. Galileo would be the first to propose a proof for the frustum of a paraboloid in a fully Archimedean style, although with a substantial change in the demonstrative structure. In 1587, still at the beginning of his career, Galileo met Clavius in Rome and gave him a copy of his demonstration for the frustum of a paraboloid. In Galileo’s correspondence of the following year, there are some letters regarding a lemma necessary for the demonstration of the center of gravity of the whole paraboloid. The nature of this correspondence and the relationship between the two will be studied in the next section. Galileo’s results on centers of gravity, which were published as an appendix to his Discorsi e dimostrazioni matematiche in 1638, concern the paraboloid and its frustum and also the pyramid, the cone, and their frusta.

The key book on centers of gravity, which according to Galileo made further research in the field unnecessary, was the De centro gravitatis solidorum libri tres (1604) by Luca Valerio (1553–1618).Footnote 32 In it Valerio brought to full fruition the ideas already present in Maurolico’s manuscript cited above.Footnote 33

Not surprisingly, Valerio’s book precluded any other attempt to determine the centers of gravity of solids. Clavius was certainly deterred by it and never published his book on centers of gravity.Footnote 34 Valerio’s work also caused Galileo’s delay in releasing his theorems on the subject, which were ready for publication by the end of the sixteenth century.

3 Another witness of the Theoremata

The witnesses known today of the Theoremata circa centrum gravitatis solidorum are

  • Galileo Galilei, Discorsi e dimostrazioni matematiche intorno a due nuove scienze ... con una Appendice del centro di gravità d’alcuni solidi (Leiden 1638, 289–314) (but numbered 306) (siglum L);

  • Los Angeles, Charles E. Young Research Library, University of California-Los Angeles, MS 170/624, folios 75–76 (siglum U);

  • Milan, Biblioteca Ambrosiana, MS A 71 Inf., folios 95–96 (siglum A).Footnote 35

Table 1 Content and witnesses

As can be seen in Table 1, the two manuscripts include only the last lemma and theorem on the conical frustum. In his edition, Favaro gave the Ambrosiana text (A) in parallel with Leiden edition (L).Footnote 36 We publish in Sect. 7 for the first time, the text contained in the UCLA manuscript (U).

For the sake of exposition, we can divide the content of the UCLA manuscript into five parts:

  • the Lemma on folio 75r, which corresponds to EN, I, 204–205;

  • a brief passage on the center of the cone: “that the center of gravity of any cone or pyramid so divides the axis that the part towards the vertex is triple the remainder was already proved by Commandino and by me in another way” [our italics];Footnote 37

  • the enunciation and beginning of the proof of the center of gravity of the frustum of a cone (75v–76r; EN, I, 205–206);Footnote 38

  • two lines of text, probably an addition or a comment by Guidobaldo, since they are underlined, as was usual when he wanted to indicate his own words;Footnote 39 and

  • the actual proof, which corresponds to the Leiden text (EN, I, 206–208).

At first sight, this manuscript does not seem to add anything significant to our knowledge of Galileo’s theory of centers of gravity: although it differs in some passages from the Leiden text, the differences are not very significant. It can however shed light on some features of the young Galileo’s research.

4 When were the Theoremata written?

The Theoremata were published only in 1638. At the end of the fourth day, Salviati presents the theorems:

These are some propositions pertaining to the center of gravity of solids which our Academician [that is, Galileo] discovered in his youth, when it appeared to him that there were still some defects in what had been left written on the subject by Federico Commandino. He thought that these propositions which you see written here might supply that which Commandino’s book left to be desired, and he applied himself to this study at the instance of the illustrious Marquis Guidobaldo del Monte, a very great mathematician of his time as shown by his various published works. Our Author gave a copy of these to that gentleman, intending to pursue the subject for other solids not touched on by Commandino. But some time later, he ran across the book of Luca Valerio, a prince of geometers, and saw that this resolved the entire subject without omitting anything; hence he went no further, though his own advances were made along quite a different road from that taken by Valerio.Footnote 40

This passage is interesting for at least three reasons. First, because it explains that Galileo decided to deal with the centers of gravity of solids to make up for what was missing in Commandino’s book. Secondly, because it explicitly states that Galileo sent a copy of these studies to Guidobaldo. The UCLA manuscript represents what remains today of the copy delivered to him. Galileo, as young man, had accepted Commandino’s challenge and began to study centers of gravity to mend some flaws present in the theorem on the frustum of a paraboloid. Then, encouraged by Guidobaldo, he continued his research. But in 1604 Luca Valerio’s De centro gravitatis solidorum libri tres was published—and this is the third reason—which put an end to Galileo’s studies on the subject. In the Discorsi there are two mentions of Luca Valerio: the one just quoted before the appendix containing the Theoremata, the other in the Second Day, after the quadrature of the parabola:

A beautiful and ingenious demonstration . . . . This proves something that Archimedes demonstrated by two different trains of many propositions, both of them admirable, and which was also demonstrated more recently by Luca Valerio, a second Archimedes according to our age, whose demonstration is given in the book he wrote on the center of gravity in solids. A book truly not to be placed below anything written by the most famous geometers of the present or all past centuries. When it was seen by our Academician [Galileo], it caused him to desist from pursuing the discoveries that he had been writing about the same subject, since he saw the whole thing so happily revealed and demonstrated by Signor Valerio.Footnote 41

But when were the Theoremata written and in what order were they proved?

Favaro dated them to 1585 on the basis of a well-known letter written by Galileo to Elia Diodati (6 December 1636).Footnote 42 According to this letter, Galileo obtained the results published in 1638 when he was “twenty-one years of age and with two years of geometrical study.”Footnote 43 So Favaro placed them in chronological order between the Iuvenilia and La bilancetta. This letter from 1636, however, is the only document on which this dating is founded. Other more direct sources suggest that Galileo had elaborated the theorems at different times and continued to work on them until the middle of 1588.

4.1 Assessment and testimonial

The first document that provides us with evidence for determining a date of composition is the Ambrosiana copy, which contains an attestation of Galileo’s authorship signed by four Florentine gentlemen and dated 12 December 1587.Footnote 44 Immediately below with the date 29 December 1587 there is also the assessment and signature of Giuseppe Moleti (1531–1588), then professor of mathematics at Padua:

On 29 December 1587, I, Giuseppe Moleti, professor of mathematics at the University of Padua, state that I have read the present lemma and theorem, which seem sound to me, and I judge their author to be a well experienced geometer. The same Giuseppe has written this in his own hand.Footnote 45

Moreover, in the MS  Gal. 72 there is an anonymous and undated letter that contains an appraisal of the lemma and the theorem on the conical frustum given orally to the sender by an unnamed friend. The sender reports that his friend “has infinite praise for the discoverer of this theorem and together with Signor Moleti judges him to be well versed in mathematics.”Footnote 46 The letter then goes on to relate his judgment of the lemma and the theorem.Footnote 47 Favaro could not offer a reliable conjecture on the identity of the sender, but suggested that the friend and assessor was perhaps Pier Antonio Cataldi (1552–1626), who held the chair of mathematics at Bologna from 1582–1626.Footnote 48

Although it is only a hypothesis, we certainly agree that the author of this judgment was very familiar with the mathematical debate concerning the centers of gravity. He cited three of the mathematicians of the time who had studied the Archimedean works and had treated the subject themselves. The first reference was to Niccolò Tartaglia’s Secundus Archimedis Tractatus.Footnote 49 The friend explained the analogy between proposition IX of second book On the Equilibrium of Planes and the lemma on frustum of a cone in meticulous and technical detail.Footnote 50 The author then cast doubt on the theorem, for the point designated as the center of gravity did not conform to the definition of center of gravity posited by Pappus and used by Guidobaldo in Le mechaniche (dal Monte (1581)), could be valid in this theorem. He finally decided to give credit to proposition XXVI of Commandino’s De centro gravitatis solidorum Commandino (1565)—the third mathematician cited—as conforming better to this definition.Footnote 51 The doubt arose probably from a misunderstanding of Pappus’s definition of center of gravity, as reported in the Italian translation of Guidobaldo’s Mechaniche, with a reference to Commandino’s version of this definition:Footnote 52

The center of gravity of any solid shape is that point within it around which are disposed on all sides parts of equal moments, so that if a plane be passed through this point cutting the said shape, it will always be divided into parts that weight equally (peseranno ugualmente) [our italics].

The assessor’s interpretation of peseranno ugualmente was wrong; with this expression Commandino did not mean that the two parts of the solid were equal in weight, but rather that they weighed equally, that is, that they were in balance with each other.Footnote 53

In any case, what matters most to us is the date of the work and its contents. The reference to Moleti’s judgment of 29 December 1587 strongly suggests that this letter was written later than the end of 1587 but, according to Favaro, before the end of 1588.Footnote 54 Furthermore, the assessor evaluated only the theorems on the conical frustum, which—according to him—were similar to Archimedes’ demonstrative style, and not the other lemmas and theorems that are found in the Leiden edition (Table 1).

Table 2 The correspondence between Galileo and Clavius

A first certain conclusion is that by 12 December 1587 Galileo had found the proof for the conical frustum and its lemma, which he then presented to his mathematical colleagues. No document proves that he already had all the proofs of the other theorems. So it is possible that the order of presentation in the Leiden edition is different from that of the discovery of the theorems.

Consistent with this is more evidence that helps to determine more precisely the entire process of composition. Along these lines, much useful information emerges from Galileo’s correspondence with Clavius (Table 2) and with Guidobaldo (Table 3).

4.2 The correspondence with Clavius

In the second half of 1587 Galileo went to Rome, where he met Clavius. At that time Galileo aspired to become professor of mathematics at the University of Bologna and was seeking approval from the most famous mathematicians of his time (Favaro 1922). To get a recommendation from Clavius, on the occasion of his visit he gave him a copy of the theorem on the frustum of a paraboloid, as emerges from a letter of 8 January 1588, in which Galileo apparently wanted to resume interrupted contacts.Footnote 55 In the letter, he sent a correction of an oversight in the theorem on the frustum of a paraboloid and asked for an opinion on a lemma necessary for the proof of the center of gravity of the whole paraboloid. The lemma in question concerns the center of gravity of a particular disposition of weights in a balance.Footnote 56 Galileo wrote to Clavius that some Florentine friends “said they were not entirely satisfied with it” (“dicono non ci haver l’intera satisfazione”).Footnote 57 On this lemma, they exchanged other two letters: Galileo’s reply of 25 February 1588, and the last letter from Clavius of 5 March 1588. At the end of this exchange, Galileo and Clavius had apparently not changed their minds. Clavius remained convinced that there was a petitio principii whereas Galileo thought that the proof was sound. This question will be discussed in detail below (see Sect. 4.4).

From these letters (Table 2) it seems that Clavius’s attitude towards Galileo’s research was ambiguous. On the one hand, he appears in his answers to be not well-disposed towards Galileo;Footnote 58 on the other he showed interest in the same research topics. In fact, a letter from Guidobaldo to Galileo of the same period (16 January 1588) states that Clavius had dealt with centers of gravity of solids and that he had proved the paraboloid frustum theorem: “Father [Clavius] then send me his proof, very different from yours [Galileo’s].”Footnote 59 Moreover, Clavius’s attitude was due not only to scientific reasons. He knew the mathematician Giovanni Antonio Magini (1555–1617), who was then in Rome. Magini was Galileo’s direct competitor for the chair of mathematics in Bologna. Clavius, when consulted by the ambassadors sent to Rome by the Senate of Bologna, had shown preference for Magini, who, in the end, was chosen for the chair.Footnote 60

In all events it is likely that the proof for the paraboloid frustum was already in a suitable form at the time of the visit to Rome, so that Galileo could leave a copy of it with Clavius. The proposition on the whole paraboloid, in contrast, was not yet available in a suitable version by the beginning January 1588 (and probably not before 5 March 1588), as is suggested by the discussion of the proof of the lemma with Clavius.

Table 3 The correspondence between Galileo and Guidobaldo

4.3 The correspondence with Guidobaldo

This is where Guidobaldo comes in. Guidobaldo’s correspondence with Galileo is wide-ranging and covers an extended period of time (Table 3). The first interesting evidence for the dating of the Theoremata appears in a letter sent by Guidobaldo to Galileo on 16 January 1588.Footnote 61 In that letter, Guidobaldo thanked Galileo for having sent him the theorem in which he had imitated Archimedes in the last propositions of On the Equilibrium of Planes. Guidobaldo was referring to the paraboloid frustum. Guidobaldo also reported that Clavius had sent him his own proof, very different from Galileo’s. Since Commandino’s De centro gravitatis solidorum ends with the demonstration for the center of gravity of the paraboloid frustum, it is conceivable that the theorem to which Guidobaldo referred is precisely that on the paraboloid frustum. The letter concludes with a request that Galileo send him more on centers of gravity (“le altre cose sui centri di gravezza”). Although not explicitly stated, it is possible that this reference is to the proof of the conical frustum, authenticated in 1587.

Another letter from Guidobaldo to Galileo, dated 24 March 1588, confirms that Galileo fulfilled Guidobaldo’s request and sent to him a proof.Footnote 62 In the following letter (28 May 1588) Guidobaldo raised doubts about the soundness of the same lemma that Galileo had discussed with Clavius:Footnote 63

Please do not omit attending to these matters on the center of gravity that you have begun, since they are most beautiful and subtle. I have seen your lemma, and to speak freely my opinion, I doubt that it begs the question [petat principium], because in the proof where it says “the center of all [the weights] is truly x, therefore x divides the lines ba and ad into the same ratio,” it seems that one could deny this conclusion.Footnote 64

These doubts were resolved only a few days later by Guidobaldo himself who, in a letter to Galileo, dated 17 June 1588, confirmed the validity of the lemma, with a proviso:

When I wrote to you about that proof of yours, it occurred to me a few days later where I had gone wrong. . . . So it seems to me that the proof is very sound, founded on that supposition, which could perhaps be proved with a little trouble.Footnote 65

Galileo, heartened by this judgment,Footnote 66 on 16 July 1588 replied to Guidobaldo and sent him the proof in which this lemma is applied, the center of gravity of the whole paraboloid. Finally, he promised him another proof, on the hyperboloid:

the center of gravity of the obtuse-angle conoid [hyperboloid] divides the axis such that the part at the vertex to the rest has the same ratio as the sum of the axis plus double the addition to the axis has to the sum of the addition and a third part of the axis.Footnote 67

This enunciation is quite different from what Luca Valerio wrote a few years later in his De centro gravitatis solidorum libri tres (1604).Footnote 68 Today there is no other trace of this theorem neither in Galileo’s correspondence nor in his printed works.

4.4 The Doubtful lemma

The lemma discussed by Galileo with Clavius and Guidobaldo concerns the center of gravity of any number of magnitudes that equally exceed one another, with the excesses equal to the least of them, hung on a balance beam at equal distances in order of weight. Galileo proved that, in this case, the point of equilibrium divides the beam in the ratio 2:1. He considered the magnitudes in two different ways, by imagining them divided and regrouped. In the first way there are five vertical magnitudes hanged at points a, c, d, e, b, from the greatest (five blocks in the figure) to the smallest (only one block). In the second we should consider the five magnitudes as disposed horizontally, hanged at points d, i, c, m, a, from the greatest (five blocks horizontally disposed) to the smallest, only one block hung at point a (see figure 1).Footnote 69 The size and position of the magnitudes along the beam remained unchanged, so that their common center of gravity also remained at the same point.Footnote 70

As we saw above in Galileo’s correspondence, “some Florentine friends,” Clavius, and even Guidobaldo were not persuaded of the soundness of the proof.Footnote 71 The Florentine friends were not satisfied with considering the magnitudes in two different ways on the same balance; according to his first letter, of 16 January 1588, however, Clavius claimed to have no problem with the reconsideration of weights, but only with the assertion that the centers of gravity of the weights considered in the two ways coincide:

this double way of considering the same magnitudes on different balances gave me no trouble, since Archimedes does almost the same thing in Proposition 6 of Book 1 of On Plane Equilibrium; but when, on balance ad, the greatest [magnitude] is hanging at d and the least at a, you now suppose that the same point x would be the point of equilibrium of the whole, as though the same point x is placed the point of equilibrium when the greatest [magnitude] hangs at a and the least at b on balance ab. This seems to be what was sought to be proved, in other words it seems to me that it begs the question. If you posit that point x is the point of equilibrium of the arm ad, as it is of the arm ab, it seems to me, according to my small judgement (being now so remote from these speculations), that your proof proceeds well.Footnote 72

Galileo tried to persuade Clavius that x, the center of gravity of the balance ab, is also the center of the balance ad:

If we stipulate that the equilibrium [point] of the composite of all the magnitudes is x when the component parts are f, g, h, k, and n, the point of equilibrium of the same composite will still be the same point x, even though I consider it to be composed of parts n, o, r, s, and t, since the point of equilibrium is one and the same of the composite and its component parts; they do not change place or size by considering them in different ways. But perhaps the diagram that I have attached will better explain my meaning, in which (and so serves my purpose) I have shown the magnitudes conjoined.Footnote 73

Galileo redrew the diagram with the “grandezze congiunte,” i.e., so that each new magnitude is now made up by small blocks joined together and not by separated columns of blocks as in the first diagram (see Fig. 1). It was an attempt to persuade Clavius of the soundness of his proof, removing the doubt caused by reconsidering the magnitudes. In the second diagram there is nothing to rearrange, the magnitudes remain the same and in the same places, only the points of suspension have changed.Footnote 74 But Galileo, despite the long explanation and the new diagram, was not successful in persuading Clavius, who replied soon after (on 5 March) reasserting his doubts. In Clavius’s last letter there are two crucial passages (EN, X, 29):

  • “mi pare che egeat demonstratione che ’l punto x resti il punto del equilibrio nella libra ad” (it seems to me that it needs be proved that the point x remains the point of equilibrium in the balance ad);

  • “ma dirà uno che ’l detto punto nella libra ad sarà un altro diverso dal x” (but one could say that the point in the balance ad would be another different from x).

Clavius remained convinced that it must prove explicitly that x remains the center of gravity. But, as Galileo tried to explain, the center of gravity remains the same because the weights had not changed their size or position: the composite body of magnitudes remained exactly the same and so therefore does the point of equilibrium.

Fig. 1
figure 1

The diagrams of the first “balance lemma”

Fig. 2
figure 2

The diagrams of the other “balance lemmas”

Guidobaldo had the same difficulty, as expressed in his letter of 28 May 1588: “Perhaps one could say that the balance ad will be divided not at x but at another point.”Footnote 75 But in the following letter (17 June), Guidobaldo said that he now understood correctly Galileo’s idea: the center of gravity is x for both considerations and so it divides the two beams in the same ratio.

it occurred to me a few days later where I had gone wrong. Since the first proof was very concise, it seemed to me that bx to xa should have had the same ratio as ax to xd, it followed that x was the center of gravity ...But it is quite the opposite, since x is the center of gravity, it follows that as bx is to xa so ax is to xd. And so it seems to me that the proof is perfectly sound, based on that assumption, which could perhaps be easily proved.Footnote 76

He persuaded himself of the soundness of the proof (“Io mi accorsi dove avevo pigliato errore”) considering two alternative lines of argument:

  1. 1.

    the beams are divided in the same ratio, therefore the centers of gravity are the same point (“avendo havere la medesima proportione bx a xa come ax a xd, che di qui ne seguitasse poi che x fusse il centro della gravità”);

  2. 2.

    the centers of gravity are at the same point, therefore the beams are divided in the same ratio (“essendo x il centro delle gravità, ne séguita che bx a xa sia come ax a xd”).

Apparently he had first thought that Galileo had argued the first, but then he realized (“ma è al contario”) that Galileo had meant the second. Assuming that the centers of gravity are the same point, he said that the argument was sound (“sì che a me pare che la dimostrazione stia benissimo, fondata in quella suppositione”), where “quella suppositione” refers to the coincidence of the centers of gravity of the two balances. This supposition he then suggested could be easily proved (“la quale si potrebbe forse provare con poca cosa”).Footnote 77

4.5 Dating the composition of Theoremata

In light of this reconstruction, Galileo first found the proof for the paraboloid frustum,Footnote 78 then that for the conical frustum and only afterwards did he pass on to the whole paraboloid.

Thanks to the correspondence with Clavius, we can assume that before March 1588 Galileo did not have a valid proof for the whole paraboloid, because of the doubtful lemma. Evidence coming from the correspondence with Guidobaldo push this date further. Only in July 1588 did Galileo send the proof for the paraboloid to his mentor, leaving us to suppose that before then and until the required lemma had been approved, he considered the theorem unsatisfactory.

A final element that concurs with the other evidence for the order of composition is the complexity of the mathematical content of these theorems. The proof for the paraboloid frustum is a simple application of the Archimedean theorem on the trapezium from On the Equilibrium of Planes, whereas the proof for the conical frustum is more complex. Galileo passed from an application in a simple case to a new proof that drew on the previous one for its inspiration.

The same holds for the proofs of the paraboloid and of the cone. Galileo devised the lemma relating to the paraboloid because, like Maurolico years earlier, he had in mind the Archimedean theorem of the center of gravity of the triangle and found a possible extension of it to the case of the paraboloid. For the cone the proof arose from noticing a similarity with the Archimedean demonstration of the center of gravity of the parabola.

From the documents discussed, and taking into account the increasing mathematical complexity of the theorems, the order of discovery would have been as follows

  • paraboloid frustum (second half of 1587, ready when Galileo went to Rome);

  • conical frustum (December 1587, from the certificate of authenticity in the Ambrosiana copy);

  • paraboloid (July 1588, from Galileo’s letter to Guidobaldo);

  • cone (post July 1588);

  • hyperboloid (post July 1588).

The study of the centers of gravity of solids and the composition of the Theoremata in a form he considered acceptable can therefore be traced back to the years 1587 and 1588. In fact, it was only at the end of 1588 that Galileo showed any intention to publish these works, an intention encouraged by Guidobaldo:

I heard also to my greatest satisfaction that you wish to publish your work on centers of gravity, which truly will bring you much honor.Footnote 79

Even when Luca Valerio’s De centro gravitatis solidorum libri tres was published in 1604, Galileo did not abandon his intention to print his early theorems. In 1607 Castelli wrote to Galileo: “I shall be awaiting the publication of your treatise On the Centers of Gravity of Solids.”Footnote 80 Some years later Galileo attempted to publish the Theoremata in the Lincean Academy with the intervention of Prince Federico Cesi. In a letter to Cesi (5 January 1613), Galileo himself, through Cesi, asked Valerio to approve the printing of his works. This request was at least curious: Galileo was aware of a conflict with the publication of Valerio but still expressed the desire to publish these works: “it would not seem good for me to throw away the not little effort that I have already made.”Footnote 81 The project however was not pursued. Even if Cesi and Valerio seemed inclined to accept Galileo’s request, nevertheless the adverb risolutamente (resolutely) hinted at Valerio’s intention to stall.Footnote 82 Not until fifty years after their elaboration in the last phase of Galileo’s scientific career, would these theorems finally see the light in the form we read today.

The correspondence with Guidobaldo provides evidence for dating not only the composition of the Theoremata but also the UCLA manuscript. There are two letters (16 November and 7 October 1588) in which Guidobaldo said he had encountered the problem of the three circles.Footnote 83 It was a problem proposed by Pappus in his Mathematical Collection and that had re-emerged thanks to Commandino’s Latin translation (Pappus (1588)).Footnote 84 The solution was extensively treated in Guidobaldo’s Meditatiunculae with the title Problema a Comandinum propositum ad Pappum pertinens dating back to 1588.Footnote 85 In the UCLA manuscript this question is mentioned twice: the first time, in the index of Meditatiunculae on folio 86r, the second time, on folio 90r, where a solution is proposed. Considering the dating of the Theoremata and of the three circles problem, the UCLA manuscript can be dated to the second half of the 1580s, at least for these texts.

5 The evolution of Galileo’s studies

The reconstruction we made confirms that between 1587 and 1588 Galileo was looking for approval for his new role as a mathematician. It is no coincidence that he elaborated and wrote the Theoremata to show his competence. In fact, although the results were not new, the proofs exhibit a full understanding of the Archimedean deductive system in general, and specifically of the contents of On the Equilibrium of Planes. In these theorems Galileo applied Archimedean techniques to more complex cases, obtaining new proofs based on the use of geometric properties. If we exclude Maurolico’s results, knowledge of which was confined to Jesuit circles, the only work that circulated freely was Commandino’s, which however had some demonstrative flaws. Galileo’s demonstrations thus allowed him to find interlocutors to establish a scientific exchange. Clavius replied with ambiguity and little enthusiasm; Guidobaldo in contrast showed a great interest in Galileo’s skills and established a lasting collaboration with him.

This collaboration is illustrated in the theorem on the conical frustum, where Guidobaldo’s transcription in U shows some interesting differences and novelties compared to the version preserved in A.

5.1 The lemma for the conical frustum

The lemma on proportional means that accompanies the theorem on the conical frustum presents only negligible differences between the three versions; but in the UCLA manuscript after the end of the proof, Galileo recalled the result for the center of gravity of the whole cone:

That the center of gravity of any cone and of any pyramid divides the axis so that the part at the vertex is triple the remainder was proven by Commandino and in a different way by me.Footnote 86

This passage is significant for two reasons: first because it is absent from L and A, and secondly because it provides information on the nature of the note transcribed by Guidobaldo. The proof of the center of gravity of the conical frustum is based on two results: the lemma proved specifically for this purpose and the theorem on the whole cone. This last result is recalled explicitly as necessary for the main theorem. The reason for the absence of this passage in L is obvious, for the proof of the whole cone is found just before the lemma. Its absence from A is strange but it can be explained: first, the result of the whole cone was already known from Commandino’s works, and secondly the Ambrosiana copy was intended only to display Galileo’s mathematical competence, and only a complex theorem could do this.Footnote 87

The passage cited above, then, seems to be of a confidential nature, as though coming from private correspondence, both for its position and for the difference in tone from what comes before and after. Its brevity, well expressed by the adverb aliter, refers to something different from what is presented here or from what is known and is in contrast to the rigorous arguments of the lemma and the theorem. The quick reference to Commandino and the expression a me recall something already known or leave it pending, with the desire to investigate the matter later.

According to Galileo and his colleagues, Commandino’s De centro gravitatis solidorum had some flaws, in particular in the proofs for the frusta. Therefore the theorem concerning the center of gravity of the whole cone, which was considered acceptable, could be neglected for the moment and taken up later.

5.2 The theorem on the conical frustum

In the enunciation of the theorem there are some differences that put U closer to L than to A (Fig. 3).

Fig. 3
figure 3

The center of gravity of the conical frustum

In U, the position of the center of gravity is expressed by the ratio between the part of the axis towards the smaller base and the remainder. In U and L the ratio is referred to the whole axis, whereas in A the ratio is given for the axis divided into four portions.

U: Cuiuslibet frusti pyramidis seu coni, plano basi aequidistante abscissi, centrum gravitatis in axe consistit, eumque ita dividit ut pars versus minorem basem ad reliquam sit ut triplum maioris basis, cum duplo spacii medii proportionalis inter basem maiorem et basem minorem, et basi minori ad triplum basis minoris cum duplo eiusdem spacii medii et basi maiori.

A: Cuiuscunque frustri pyramidis seu coni, plano basi aequidixtante abscissi, centrum gravitatis in axe consistit, ita ut prius ab eo utrinque quarta sui parte dempta, centrum gravitatis in reliqua consistit; eanque sic dividit, ut pars versus minorem basem ad reliquam eandem habeat rationem, quam spacium quod basium sit medium proportionale cum duplo maioris basis habet ad idem spacium inter bases proportionale cum duplo minoris basis [our italics].

If we designate (following Galileo’s notation in U) the smaller base with R, the greater with B and the proportional mean between the two bases with C, then in L and U the center of gravity o of \(\mathcal {F}\) frustum will divide the ud axis in a such way that

$$\begin{aligned} uo:od=(3B+2C+R):(3R+2C+B) \end{aligned}$$

On the other hand, in A, the axis of the frustum ud is divided into four parts, and the center of gravity o will be on the two middle quarters mr according to the ratio:

$$\begin{aligned} mo:or=(2B+C):(2R+C) \end{aligned}$$

Consistent with the enunciation, the settings out and the first part of the proofs also show these differences.Footnote 88 Before going into some details about the proofs, we should note that U has two passages not present in the other witnesses. The first is found in the setting out:

Frusti autem maior basis aequalis sit spacio B, minor vero R. Spaciorum autem B R medium esto proportionale C.

The letters B R C are introduced both into the text and into the diagram to designate areas equal to the bases (see Fig. 4). In L and A periphrases are used to designate these areas.Footnote 89

Fig. 4
figure 4

The diagram in the UCLA manuscript U

The second passage unique to U is another linking sentence, right at the end of the determination and before the beginning of the actual proof:

But it is obvious that the center of gravity of the frustum lies on the axis, since the centers of gravity of the whole cone or pyramid, and of the abscissa of the cone or pyramid, lie on the same axis.Footnote 90

This comment, which is underlined in the manuscript, was probably an addition by Guidobaldo himself and does not make a substantial contribution to the argument of the theorem.

Once the setting out is finished, the proofs in the three witnesses proceed in the same manner. Four auxiliary lines in continuous proportion are introduced so that a specific lemma can be applied.Footnote 91 It is then possible to prove that point n is the center of gravity of the whole cone \(\mathcal {C}\).Footnote 92 Next point i is found as the center of gravity of the smaller cone \(\mathcal {K}\), the difference between \(\mathcal {C}\) and \(\mathcal {F}\) (see Fig. 5).

Fig. 5
figure 5

The proof of the center of gravity of the frustum.

The proof is thus reduced to proving that \(in:no=\mathcal {F}:\mathcal {K}\).Footnote 93

This proportion is obtained by the application of the law of the lever (On the Equilibrium of Planes, I.8) to the cones \(\mathcal {C}\) and \(\mathcal {K}\).Footnote 94 In fact, given the whole cone \(\mathcal {C}\) with center of gravity n, and the cone part of it \(\mathcal {K}\) with center of gravity i, the center of gravity of their difference (frustum \(\mathcal {F}\)) will be a point o on in such that \(no:in=\mathcal {K}:\mathcal {F}\).

L and U thus offer the same mathematical point of view, with two differences: in the manuscript

  1. 1.

    the whole discourse seems to be more amalgamated as can be seen from the connecting sentences between the parts;Footnote 95 and

  2. 2.

    there is an attempt to simplify some periphrases.Footnote 96

A in our opinion is the oldest version and presents a more Archimedean determination. Archimedes (in On Equilibrium of Planes II.10) divided the axis of the mixtilinear trapezium into five equal parts, and showed that the center of gravity lies in the middle part and divides it in a certain ratio.Footnote 97 Similarly, Galileo divided the axis of the conical frustum into four equal parts and proved that the center of gravity lies in the two middle parts and divides them in a certain ratio.

5.3 Reasons for a change?

Why this difference of style between the various versions of the conical frustum?

Actually, a similar change occurs in the theorem on the center of gravity of the frustum of a paraboloid in L.

In this case, Galileo also expounded the proposition by taking as his model the Archimedean formulation of the mixtilinear trapezium (On the Equilibrium of Planes, II.10): he divided the axis into three equal parts and proved that the center of gravity lies in the middle part and divides it according to a certain ratio.Footnote 98 The proof, however, closely follows Archimedes’ proof of the center of gravity of the trapezium, which presents an enunciation similar to that of the Leiden version and of the UCLA manuscript described above.Footnote 99 Galileo, aware of the demonstrative analogies between the frustum of a paraboloid and the trapezium, realized this stylistic difference and at the end of the demonstration added the following note:

Therefore it is clear that the center of gravity of frustum ULMC is point I, and the axis is so divided [by it] that the part toward the smaller base is to the part toward the larger base as double the larger base plus the smaller is to double the smaller plus the larger. Which is the proposition, but more elegantly expressed [out italics].Footnote 100

He considered an enunciation nearer to the Archimedean style “more elegantly expressed” (elegantius). The same choice was repeated for the conical frustum in U: the first “less elegant” statement survived only in A, the oldest version.

By putting together what emerges from the dating and from the mathematical analysis, it is possible to conclude that Galileo proved the theorems at different times and in a different order from the one he used when he belatedly published the work. The oldest text, unrevised stylistically, is preserved in A, whereas U takes an intermediate position between A and L.

The link between the young Galileo and Guidobaldo was not hierarchical but one of equality: Guidobaldo deeply esteemed the Galileo’s results on centers of gravity, deeming them worthy of publication. This emerges both from the UCLA manuscript, which preserves Guidobaldo’s copy of the notes sent to him by Galileo, and from their correspondence. In his letters, Guidobaldo constantly encouraged Galileo to continue his mathematical studies, always waiting for new findings.Footnote 101

Galileo’s studies of the centers of gravity were part of a research field in which the most important mathematicians of the time had already expressed themselves, achieving considerable results. Even if Galileo’s proofs fit into this tradition, however, they clearly revealed his affinity with the Archimedean way of thinking. Galileo not only showed he had read and understood On the Equilibrium of Planes but he also adapted its Archimedean proofs to more complex cases. Galileo was faithful to his model in the individual arguments, in the presentation of the results obtained and even in style.

6 Some conclusions

As we have seen, Galileo began to deal with centers of gravity of solids to show his mathematical competence. He came into a research field in which the results achieved by his contemporary colleagues were not fully satisfactory.

The Theoremata does not seem to have been born in the same order as the Leiden printing, and their composition responded to different needs: Galileo first wanted to enter into the field of mathematical research, accepting the challenge thrown by Commandino; besides this, he aspired to become a mathematician, showing that he knew how to extend Archimedean ideas to more complex cases. Thus, at the beginning, not fully satisfied with the treatment by his contemporaries, he solved the theorems on the center of gravity of the frusta, and only afterwards did he go on to the centers of the whole solids, proposing a new approach. The idea of publishing these theorems dates to the end of 1588, when he believed he had produced an acceptable work.

The comparison between the three versions affords a glimpse into some of Galileo’s traits as a young mathematician. He was a careful and deep expert in Archimedes’ mathematics. He was aware that the ideas and principles of Archimedes’ work could be successfully applied to solids, and that it was only necessary to change the lemmas accordingly. Galileo was following in the footsteps of Archimedes who did the same when he built the proof for the portion of a parabola on that for the trapezium.

Finally, the Ambrosiana copy, the oldest of the three extant copies, shows stylistic differences from both the UCLA manuscript and the Leiden printing. It seems from this that Galileo wanted to follow Archimedes not only in mathematics but also in style, using in his own proofs the same elegant stylistic features that he had found in Archimedes.

7 Appendix: The text of the UCLA manuscript

7.1 Description of the codex

Manuscript U (Los Angeles, Charles E. Young Research Library, University of California-Los Angeles, MS 170/624), is divided into three parts. For our purpose only the second part, mainly written by Guidobaldo, is relevant.Footnote 102

This section of the manuscript is made up of sheets of different kinds of paper with different dimensions, written in different hands and inks, and on various topics. It was assembled from miscellaneous materials written at various times.

It consists of 21 folios, numbered in the upper right corner 75–91: four folios are numbered \(83{-}1^{\mathrm{o}}\), \(83{-}2^{\mathrm{o}}\), \(83{-}3^{\mathrm{o}}\) \(83{-}4^{\mathrm{o}}\), the last folio (92) is not numbered.Footnote 103 The text is written mostly in Latin, although folios 79–82, 85 and 91 are in Italian.Footnote 104 There are at least four hands: Guidobaldo wrote most of the folios, except folios 79, \(83{-}3^{\mathrm{o}}\), 89 and 91v. The manuscript is not dated, but folio 83 contains astronomical data referring to October and November 1580.Footnote 105

On folio 84r there is a reference to a diagram (ut in secunda figura) on folio 82r. For this reason, it is probable that folios 82 and 84 form a bifolio.Footnote 106

On the basis of content, paper dimensions, ink and internal references it is possible to guess that folios 75–76, 77–78, 80–81, 82–84 and 87–88 also form bifolios.

7.2 Content

ff. 75–76:

Galileo’s proof for the conical frustum with two geometrical diagrams (76v blank);

ff. 77–78, \(83{-}3^{\mathrm{o}}\):

On 77r an extract from De limitibus constituendis by Hyginus: “Verba Hygeni de limitibus constit. Pag. 117.” Quotation (and diagram) copied from pages 117–118 of Hyginus (1554). On \(83{-}3^{\mathrm{o}}\) the same text as 77r is repeated in a different hand. Folio \(83{-}3^{\mathrm{o}}\)v, however, has a passage not present on 77r: “Eisdem ...convenit,” with another geometrical diagram from the same edition (page 118, lines 13–16); 77v and 78 contain notes and diagrams by Guidobaldo on Hyginus: “Haec Hygeni verba una cum figura hoc modo corrigi posse videntur” (77v); “Huius constructionis demonstratio” (78r) and “Praxis” (78v).Footnote 107

f. 79, 80–81:

Two problems “Proposti dal S. Marchese di Carrara”; solutions to the problems are proposed on 80–81.Footnote 108

f. 82r:

“Sia il cono scaleno abc ...” two geometrical diagrams

f. 83 \(1^{\mathrm{o}}\)\(2^{\mathrm{o}}\):

“Multi spernunt ...,” a theoretical text on mathematics.

f. 83–\(4^{\mathrm{o}}\):

Astronomical data for a comet dated 1580 at the top of the page. The observations are on October 10th, October 16th and November 20th.

f. 84r:

“Propositio 8. Problema. Duabus datis rectis lineis in eodem plano non existentibus lineam ambobi perpendicularem ducere.” This folio has no mathematical diagram but instead notes: “ut in secunda figura,” in reference to the second figure on 82r.

f. 85r:

Constructions of the three conic sections (with four diagrams) written in Italian. A leaf is attached to the folio, partially covering the text. At the end of the folio (apparently in different ink) there are two notes: “verticali perché tutti passano per il vertice che è il zenit” and “Del Galileo.”

f. 86r:

A list in Guidobaldo’s hand of some topics treated in the Meditatiunculae (86v blank).Footnote 109

ff. 87–88:

Bound upside down, notes by Guidobaldo on some propositions from Valerio (1582). The text starts on 88v with proposition XXII and continues on 88r with proposition XXIII, and 87v with proposition XXIV (XXIIII, in the manuscript); and ends on 87r with proposition 8 (=VIII).

f. 89:

Another list of topics in the Meditatiunculae (not autograph).Footnote 110

f. 90r:

Pappus’s three circles problem “Tribus datis circulis inaequalis qui se non contingant ...circulum describere qui omnes contingat.”Footnote 111

f. 91r:

“Sia A l’occhio, B il punto della distanza ...” No geometrical diagram, although two diagrams are cited in the text: “avvertendo che nella prima figura”; “sia nella seconda figura.”

f. 91v:

At the bottom of the page, upside down, there is a short letter (six lines of text, in Italian) quite fainted and almost unreadable; in this letter, the name Guidobaldo appears twice.

f. \(92^{*}\):

On the recto and the verso of this unnumbered leaf, two geometrical diagrams of an ellipse are found.

7.2.1 A possible dating for the manuscript

It is possible to conjecture that this part of the manuscript was written mainly around 1580–1590, in particular because

  • folio 83 contains astronomical data of a comet recorded in October and November 1580;Footnote 112

  • folios 87–88 report some theorems from Valerio (1582);

  • the folios on the center of gravity of the conical frustum are datable to 1587-1588, as we have seen; and

  • the part of the Meditatiunculae that shows connections with this manuscript can be dated between 1586–87 and 1593.Footnote 113

7.3 Editorial criteria

In the edition we have written out abbreviations and abridgements; for example prima for “p.a,” quarta for “4.a,” dupla for “2pla,” and so on. Punctuation, capitalization and use of the letters “u” “v” and “i” “j” have been adjusted to modern usage. Concerning the mathematical lettering, we have adopted the style of Favaro’s Edizione nazionale and used small letters in italics, both in the text and in the diagrams.Footnote 114 Reference to the pagination of the witnesses is in the margin of the page. The text is subdivided by paragraph numbers in smaller, boldface type.

We have not recorded in the apparatus the graphical variants and misprints that we report here: spacium U A spatium L; basem U A basin L. The copist of A sometimes writes either aequidixtante or aequidistancte, and frustrum (in one occurrence fruxtrum). There are two misprints in mathematical lettering: hxk for hx xk; abo for “ab o,” and some others less important.

The UCLA manuscript has some erasures and imperfections; we have noted the most important ones, leaving out those that involve only one letter. For example, at the top of folio 76r there is, at least in our photographic reproduction, a patch that covers the space of a few words.

The diagrams are similar in the three witnesses and we have reproduced the diagrams in U. As noted above (see Sect. 5.2) U has three circles representing the areas of the greater base, the smaller base and their mean proportional.

7.4 Sources and internal references

In the UCLA manuscript there are three mathematical references:

  1. 1.

    per conversam \(24^{ae}\) quinti;Footnote 115

  2. 2.

    A Comandino et aliter a me demonstratum est;

  3. 3.

    per Lemma praecedens.

The first reference is to Euclid, Elements, book 5, proposition 24. The second is to Commandino’s theorem on the center of gravity of the cone, proposition 18 of his De centro gravitatis solidorum (Commandino 1565), folios 27v-30r. The third is an internal reference to the Lemma at the beginning of the text.

In the Ambrosiana manuscript there are two other references in the margin:

  1. 1.

    “11 et 12.6”; and

  2. 2.

    “20.6 vel 2.12 vel 7 Conoid. Archim.”

The first two refer to Euclid, Elemets, VI.11 and VI.12, where the existence of the third and the fourth proportional is proved.Footnote 116 The second three refer to Euclid, Elements, VI.20 and XII.2, and Archimedes, On Conoids and Sphaeroids, proposition 6.Footnote 117

SIGLA

  1. U

    Los Angeles, Charles E. Young Research Library, University of California-Los Angeles, MS 170/624, folios 75–76

  2. L

    Editio princeps: Galileo Galilei, Discorsi e dimostrazioni matematiche intorno a due nuove scienze ...con una Appendice del centro di gravità d’alcuni solidi (Leiden, 1638), 289–314 (but numbered 306)

  3. A

    Milan, Biblioteca Ambrosiana, MS A 71 Inf, folios 95–96

  4. Favaro

    Edizione Nazionale delle Opere di Galileo

  5. del.

    delevit

  6. om.

    omisit

  7. post corr.

    post corectionem

  8. add.

    addidit

  9. in marg.

    in margine

8 Lemma. Galileus

Lemma. Galileus U Lemma A om. L

Si fuerint quatuor lineae continue,Footnote 119 proportionales et quam rationem habet minima earum ad excessum quo maxima minimam superat, eandem habuerit linea quaedam sumpta ad \(\frac{3}{4}\) excessus quo maxima secundam superat, quam autem rationem habet linea his aequalis maximae, duplaeFootnote 120 secundae et triplae tertiae ad lineam aequalem quadruplae maximae, quadruplae secundae et quadruplae tertiae, eandemFootnote 121 habuerit alia quaedam sumpta ad excessum quo maxima secundam superat, erunt istae duae lineae simul sumptae quarta pars maximaeFootnote 122 proportionalium.

figure a

Sint enim quatuor lineae continueFootnote 123 proportionales ab bc bd be et quam rationem habet be ad ea eandem habeat fg ad \(\frac{3}{4}\) acFootnote 124, quam autem rationem habet linea aequalis ab etFootnote 125 duplae bc et triplae bd ad aequalem quadruplae ipsarum ab bc bd, hanc habeat hg ad ac. OstendendumFootnote 126 est hf quartam esse partem ipsius ab.

Quia igitur ab bc bd be sunt | continueFootnote 127 proportionales in eadem ratione erunt etiam ac cd de et ut quadrupla ipsarum ab bc bd ad ab cum dupla bc et tripla bd ita quadrupla ipsarum ac cd de, hoc est quadrupla ipsius ae, ad ac cum dupla cd et tripla de et sic est ac ad hg. Ergo ut tripla ipsiusFootnote 128ae ad ac cum dupla cd et tripla de ita \(\frac{3}{4}\) ipsius ac ad hg. Est autem ut tripla ae ad triplam eb ita \(\frac{3}{4}\) ac ad gf. Ergo, per conversam \(24^{\mathrm{ae}}\) quintiFootnote 129, ut tripla ae ad ac cum dupla cd et tripla db ita \(\frac{3}{4}\) ipsius ac ad hf, et ut quadrupla ae ad ac cum dupla cd et tripla db, hoc est ad ab cum cb et bd, ita ac ad hf et permutando, ut quadrupla ae ad ac ita ab cum cb et bd ad hf, ut autem ac ad ae ita ab ad ab cum cb et bd. Ergo ex aequali proportioneFootnote 130 perturbata ut quadrupla ae ad ae ita ab ad hf: quare constat hf quartam esse partem ipsius ab.

CuiuslibetFootnote 131 coni et cuiuslibet pyramidis centrum gravitatis axem dividere ut pars ad verticem reliquae sit tripla, a Comandino et aliter a me demonstratum est.

CuiuslibetFootnote 132 frusti pyramidis seu coni, plano basi aequidistante abscissiFootnote 133, centrum gravitatis in axe consistit, eumque itaFootnote 134 dividit ut pars versus minorem basem ad reliquam sitFootnote 135 ut triplumFootnote 136 maioris basis, cum duplo spacii medii proportionalisFootnote 137 inter basem maiorem et basemFootnote 138 minorem, etFootnote 139 basi minori ad triplumFootnote 140 basis minorisFootnote 141 cum duplo eiusdemFootnote 142 spacii medii etFootnote 143 basi maiori.

figure b

SitFootnote 144 frustum cuius axis du sectum | a cono vel pyramide cuius axis da. FrustiFootnote 145 autem maior basis aequalis sit spacio B, minor vero R. Spaciorum autem B R medium esto proportionale C. Frusti autem du axis dividatur in o, ita ut pars uo ad reliquam od eandem habeat rationem quam tres B cum duobus C et unum R ad tres R cum duobus C et unum B.

DicoFootnote 146o centrum gravitatis frusti cuius axis udFootnote 147 existere. QuodFootnote 148 autem centrum gravitatis frusti in axe consistat, manifestum est, cum totius coni vel pyramidis, et coni vel pyramidis abscissae centra gravitatum in eodem axe consistant.

Sit um quarta pars ipsius udFootnote 149. Exponatur linea hx ipsiFootnote 150ad aequalis sitque kx aequalis au, ipsarum vero hx xk tertia proportionalis sit xl, et quarta xs. Et quam rationem habet hs ad sx eandemFootnote 151 habeat md ad lineam sumptam ab o versus a, quae sit on. Et quia maior basis ad eam quae inter maiorem et minorem est media proportionalis, est ut da adFootnote 152au, hoc est ut hx ad xk, dicta au|tem media ad minorem est ut kxFootnote 153 ad xl (sunt enim hx xk xl continue proportionales)Footnote 154, erunt maior, media et minor basesFootnote 155 in eadem ratione et lineae hx xk xl.

Quare triplaFootnote 156 maioris basis cum dupla mediae et minima ad triplam minimae cum dupla mediae et maioriFootnote 157, hoc est ut uo ad od, ita tripla hx cum dupla kxFootnote 158 et xl ad triplam xl cum dupla xk et xh, et componendo et convertendo erit od ad du ut hx cum dupla xk et triplaFootnote 159xl ad quadruplam ipsarum hx xk xl.

Sunt itaqueFootnote 160 quatuor lineae continueFootnote 161 proportionales hx xk xl xs; et quam rationem habet xs ad sh hanc habet linea quaedam sumpta no ad \(\frac{3}{4}\) ipsius du, nempe ad dm, hoc est ad \(\frac{3}{4}\) ipsius hk. Quam autem U:habet rationemFootnote 162hx cum dupla xk et tripla xl ad quadruplam ipsarum hx xk xl, eandem habet alia quaedamFootnote 163 sumpta od ad du, hoc est ad hk. Ergo per lemma praecedensFootnote 164dn erit quarta pars ipsius | hx, hoc estFootnote 165ad. Quare punctum n | erit gravitatis centrum coni, vel pyramidis, cuius axis adFootnote 166. Sit pyramidis vel coni cuius axis au centrum gravitatis i. Constat igitur centrum gravitatis frusti esse in linea inFootnote 167 ad partes n extensa, in eoque eius puncto quodFootnote 168 cum puncto n lineam intercipiat ad quam in eam | habeat rationem, quam abscissum frustum habet ad pyramidem, vel conum, cuius axis auFootnote 169.

Ostendendum itaque restat in ad no eandem habere rationem, quam frustum ad conum cuius axis au. Est autem ut conus cuius axis da ad conum cuius axis au, ita cubus da ad cubum au, hoc est cubus hx ad cubum xk. Haec autem eadem est ratioFootnote 170 quam habet hx ad xs, quare dividendo ut hs ad sx ita erit frustum cuius axis du ad conum vel pyramidem cuius axis ua.

Est autem utFootnote 171hs ad sx ita mdFootnote 172 ad on, quare frustum ad conum velFootnote 173 pyramidem cuius axis au est ut md ad no. Et quia an est \(\frac{3}{4}\) ipsius ad, ai autemFootnote 174\(\frac{3}{4}\) ipsius au, erit reliqua in \(\frac{3}{4}\) reliquae ud. Quare in aequalis erit ipsi md. Et demonstratum est md ad no esse ut frustum ad conum vel pyramidem cuius axisFootnote 175au. Constat ergo hanc eandem rationem habere etiam in ad no. Quare patet propositum.