Abstract
After Galileo’s death in the mid-sevententh century, mixed mathematics accelerated its race to conquer all the areas of natural philosophy, with the emergence of what was called physico-mathematica. The process did not depend only on Galileo, but it was part of a long wave that started in the Renaissance with the revitalization of mathematics consequences and causes of European technological development. Of this long wave Galileo was among those who rode the highest billows. One component of this process was the establishment of a strong empiricist component among mathematicians and philosophers of nature, with a relevant space attributed to experimental laboratory practice. This empiricist component is effectively exemplified by the birth of the Academia del cimento and the Royal society. There were, however, characters who went beyond experimental practice. They were the like of Borelli, Baliani, Mersenne, Hooke, and Boyle. They used the results of contrived experiments to develop new branches of physico-mathematica and were crucial for the mathematicians would become the new natural philosophers.
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Notes
- 1.
p. 101.
- 2.
The most extensive treatment of Borelli’s life is in Angelo Fabroni, Vitae italorum doctrina excellentium, II (Pisa, 1778), 222–324.
- 3.
pp. 74–75.
- 4.
pp. 437–438.
- 5.
p. 3.
- 6.
In the following I translate always with “force” the Latin terms vis, virtus, facultas, used by Borelli.
- 7.
p. 272.
- 8.
p. 4.
- 9.
pp. 45–46.
- 10.
p. 77.
- 11.
p. 47.
- 12.
pp. 48–49. Translation in [110].
- 13.
p. 49.
- 14.
pp. 60–61.
- 15.
p. 30.
- 16.
pp. 59–62.
- 17.
p. 56.
- 18.
p. 3.
- 19.
pp. 61–62. Translation in [110].
- 20.
pp. 663-64.
- 21.
p. 63.
- 22.
p. 65.
- 23.
p. 67.
- 24.
pp. 274–275.
- 25.
pp. 75–76.
- 26.
pp. 78. Translation in [110].
- 27.
Letter to the Queen Christina.
- 28.
Proemium. Translation in [32].
- 29.
Pars I, p. 30.
- 30.
p. 1.
- 31.
Pars II, p. 96.
- 32.
Pars I, p. 13. Translation in [32].
- 33.
Part I, Proposition 9, p. 11.
- 34.
Part I, p.31.
- 35.
Part I, Proposition 12 pp. 13–14.
- 36.
p. 162.
- 37.
pp. 170–171.
- 38.
Part I, Proposition 114, p. 132. Translation in [32].
- 39.
p. 166.
- 40.
Part II, Proposition 14, p. 16.
- 41.
Part II, Proposition 22–26, pp. 32–36.
- 42.
p. 43. Translation in [32].
- 43.
Pars I, p. 27. Translation in [32].
- 44.
p. 21. Translation in [32].
- 45.
Pars I, p.116. Translation adapted from [32].
- 46.
p. 47.
- 47.
p. 678.
- 48.
p. 261.
- 49.
vol. 11, p. 610.
- 50.
pp. 18–31.
- 51.
I had no access to the 1647 edition therefore reference is to [10].
- 52.
pp. 5–6.
- 53.
p. 5.
- 54.
p. 8.
- 55.
pp.10–12.
- 56.
pp. 14–17.
- 57.
- 58.
vol. 4, pp. 313–314.
- 59.
vol. 18, pp. 12–13.
- 60.
Baliani’s reply is to Galileo’s lost letter of June 20th, 1639; [140], p. 141.
- 61.
vol. 18, p. 69.
- 62.
pp. 32–36.
- 63.
Cavalieri seemed to appreciate Baliani’s mathematical approach [12], pp. 34–35.
- 64.
- 65.
p. 53.
- 66.
p. 54.
- 67.
p. 139.
- 68.
p. 140.
- 69.
vol. 14, pp. 343–344.
- 70.
For instance, Galileo in his Dialogo sopra i due massimi sistemi declared that a heavy body will pass 100 braccia in 5 seconds, in a free fall, [83], vol. 7, p. 250. Assuming that 1 braccio is about 0.55 m (this is a current estimate), the acceleration of gravity (modern term) would be about 4.5 m/s\(^2\), much less than the true value (9.8 m/s\(^2\)) and of the value found by other experimentalists such as Mersenne ; see, for instance, [107].
- 71.
Letter to Galileo August 19th, 1639. [83], vol. 18, p. 87.
- 72.
pp. 41–56.
- 73.
p. 27.
- 74.
vol. 13, pp. 348–349.
- 75.
- 76.
p. 267.
- 77.
p. 97.
- 78.
To note that in the quoted letter to Galileo , July 1st, 1639, Baliani listed the components of mixed mathematics, including astronomy.
- 79.
pp. 97–98.
- 80.
p. 101.
- 81.
p. 99.
- 82.
p. 113.
- 83.
pp. 265–270.
- 84.
- 85.
p. 204.
- 86.
Preface, not numbered pages.
- 87.
p. 97.
- 88.
pp. 39–57.
- 89.
pp. 43–44.
- 90.
p. 229.
- 91.
p. 354.
- 92.
p. 226.
- 93.
pp. 5–6. Translation in [123].
- 94.
pp. 158–162.
- 95.
p. 229.
- 96.
pp. 194–205.
- 97.
p. 120.
- 98.
It had become common to give the space of fall in 1 s. This value played a role similar to that played today by the acceleration of gravity. A modern physicist – and also a high school student – applying the now well-known formula: \(s = 1/2 gt^ 2 \), recognizes that the space s of fall in a second is half the acceleration gravity g. At the time of Mersenne this reasoning was not possible simply because the concept of acceleration as well- defined kinematic magnitude did not exist until the works of Leonhard Euler in the first half of the eighteenth century.
- 99.
For a Paris foot it can be assumed a length of 32.5 cm. For a Paris pound \(=\) 16 ounces it can be assumed in the mass of 0.489.5 kg.
- 100.
vol. 1, p. 86.
- 101.
vol. 1, p. 87.
- 102.
vol. 7, p. 250. Galileo himself had doubts on the validity of his numbers. In fact, in a marginal addition to his own copy of the Dialogue he provided a much improved value. He had Simplicio say that a lead ball of 100 pounds would fall over 100 braccia in four pulse beats, a much more accurate value. It seems plausible that Galileo had tried the experiment after the 1639 letter to Baliani, this time directly from a high tower [20], p. 176.
- 103.
In an appendix, Mersenne referred to the opinion of Nicolas-Claude Fabri de Peiresc (1580–1637) according to whom Galileo’s braccio should be greater, equal to 1.80 feet, but, said Mersenne , the result did not change substantially.
- 104.
vol. 1, pp. 86–87.
- 105.
For the value of CT Mersenne arrived at a result that expressed with modern symbolism is given by CT = CB \(\sin \widehat{\text {BAC}}\), which is correct. This result was already obtained by Galileo and reported on the first day of the Dialogo sopra i due massimi sistemi del mondo [83], vol. 7, p. 51. From Galileo Mersenne also resumed all the figures that relate to the inclined plane.
- 106.
vol. 1, p. 111.
- 107.
It should be remembered that Galileo discussed, in published work, his experiments on the fall along the inclined plane not before the Discorsi e dimostrazioni matematiche sopra due nuove scienze of 1638, whereas here Mersenne is writing in 1636.
- 108.
vol. 1, p. 112.
- 109.
vol. 1, p. 112.
- 110.
p. 112.
- 111.
Phenomena ballistica, p. 52. Translation in [150].
- 112.
pp. 217–219.
- 113.
pp. 125–127.
- 114.
p. 135.
- 115.
p. 136.
- 116.
Applying the relation \(T = 2\pi \sqrt{l/g}\) valid for small oscillations, assuming \(l = 3\times 0.325 = 0.975\) m, g = 9.8 m/s\(^2\) one obtains \(T = 1.98\) s. A quarter of a period thus is about 0.5 s.
- 117.
pp. 75.
- 118.
p. 153. Calculating the theoretical period of a pendulum – according to modern theories – starting with an angle of 90 degrees, it is found that it exceeds by about 20% that of small oscillations. A pendulum of \(2\,\frac{1}{6} = 2.17\) feet has a period for small oscillations of \(\sqrt{(2.17/3)} = 0.85\) times less than the period of the pendulum of length 3 feet; but in large oscillations it has a period approximately equal to that of 3 feet in small oscillations. The numerical value of 2.17 feet, which Mersenne proposed without much emphasis is surprisingly close to reality and indicates either that Mersenne was lucky or that his experimental mode was very refined. I comment later that it is not easy to choose between these options.
- 119.
11/7 is the approximation used by Mersenne for \( \pi / 2 \).
- 120.
Actually Mersenne referred explicitly only to Baliani , citing him by name, and his De moti naturali gravium solidorum et liquidorum, Book 6, of 1646 [135], p. 156.
- 121.
p. 111.
- 122.
vol. 17, p. 281.
- 123.
vol. 1, p. 278.
- 124.
vol. 1, Livre premier des mouvemens, p. 14.
- 125.
The same opinion of Galileo ; whereas Descartes and Aristotle considered the speed of light infinite.
- 126.
vol. 1, Livre premier des mouvemens, p. 50.
- 127.
vol. 1, Livre premier des mouvemens, p. 48.
- 128.
vol. 1, Livre troisieme des mouvemens, p. 217.
- 129.
vol. 1, Livre premier des mouvemens, p. 52.
- 130.
vol. 1, Livre troisieme des mouvemens, pp. 213–214.
The distance \(2\times 485 = 970\) feet corresponds to a speed of 315.25 m/s, or of 1135 km/h, a value slightly lower than that measured today in ideal environmental conditions which is around 1200 Km per hour (about 170 toises per second). Mersenne also commented on the result he had reported elsewhere, a value of 150–180 feet for the echo of one syllable, thus for the time of a seventh of second [132], vol. 1, Livre premier des mouvemens, p. 52. The extent of \( 485 \times 2 \) standing for seven syllables provides 138 feet for a syllable, a significantly lower value.
- 131.
vol. 1, Livre troisieme des mouvements, p. 214.
- 132.
The lieue is a unity of length corresponding to two miles, or about a one-hour walk. For Mersenne a lieue was 2500 toises and thus \(2500\times 6\times 0.325 = 4875\) m.
- 133.
vol. 1, Livre troisieme des mouvemens, p. 214. Actually there are some incongruities in Mersenne’s text. First, he said that the speed of the sound is 12 toises per second, that is, 72 feet per second, instead of 69 feet, as stated before. Second, there should be a typo, because Mersenne said that the time necessary to pronounce 208 syllables is 9 s instead of 29, corresponding to 1/7 of second per syllable.
- 134.
vol. 1, Livre troisieme des mouvemens, p. 220.
- 135.
Ballistica et acontismologia, pp. 138–140.
- 136.
p. 38.
- 137.
pp. 15–16.
- 138.
Praefatio, first page.
- 139.
p. 246.
- 140.
p. 40.
- 141.
p. 53.
- 142.
vol. 11, p. 126. Translation in [61]
- 143.
pp. 16–19.
- 144.
p. 208.
- 145.
p. 49.
- 146.
p. 165.
- 147.
pp.150–151.
- 148.
vol. 1, p. 7.
- 149.
pp. 2–3.
- 150.
pp. 33–35.
- 151.
pp. 34–38.
- 152.
pp. 499–500.
- 153.
Chapter 3.
- 154.
Pars posterior, p. 235.
- 155.
p. I, in the subtitle.
- 156.
vol. 1, p. XIX.
- 157.
vol. 2, p. 419.
- 158.
p. 86.
- 159.
Pars prior, pp. 535–536.
- 160.
Pars posterior,“An Proportiones motuum caelestium, sint scibiles a nobis in hac vita & effabiles, & An rationales omnes, an vero alique irrationales; ubi de Revolutionibus eorum omnium in idem”, p. 269.
- 161.
p. 5.
- 162.
Pars prior, pp. 89–91.
- 163.
Pars posterior, pp. 381–397.
- 164.
Pars posterior, p. 385.
- 165.
p. 83.
- 166.
Pars posterior, p. 383.
- 167.
The measure of the Roman foot to which Riccioli is concerned can be deduced by a half foot drawn in scale 1:1 in the Almagestum novum [159], Pars prior, p. 58, resulting in about 15.4 cm. Thus Riccioli’s Roman foot is 30.8 cm. This value can be confirmed by noting that Riccioli said the Torre degli Asinelli was 312 feet high and that today the height estimate is of 97 m; which gives for a Roman foot the value of 31 cm, very close to 30.8. Considering the error of measurement both in the height of the tower and the length of drawing, the two values confirm each other.
- 168.
Pars posterior, p. 385.
- 169.
Note that time is expressed in seconds (\(''\)) and sixtieths of second (\('''\), or thirds), instead of seconds and tenths of second as usual today.
- 170.
Pars posterior, p. 386.
- 171.
Corresponding to value of the acceleration of gravity of 8.87, 9.24, 9.44 m/s\(^2\), a bit lower the real value measured today in vacuum \(\approx \)9.8 m/s\(^2\).
- 172.
See for instance vol. 17, p. 281. Here a value of 15 feet and 7.5 inches, equal to 15, 625 feet is proposed, basing on the measurement of the period of a conic pendulum. Assuming for Huygens’s foot a value equal to 31.38 cm – slightly greater that the Roman foot – this gives a value \(g=9.79\) m/s\(^2\) [180], p. 32.
- 173.
Pars posterior, p. 386.
- 174.
Chapter 3.
- 175.
Pars prior, p. 90.
- 176.
For example, if reference is made to fall from 60 feet, assuming an acceleration of about 30 feet/s\(^2\) (9.8 m/s\(^ 2\)), the ball reaches the ground with the speed of about 60 feet per second. If it is supposed to be able to appreciate a half-oscillation of the pendulum, the error in the time measurement could be about 1/12 of a second, which leads to not distinguish falls that occur in a 5 (\(=\)60/12) foot fork. Notice that for the second and third series of tests the height of fall in the first time interval, could be determined from the first test of the first series. This would have given heights of fall equal to \(10 \times (6/5)^2= 14.4\), instead of 15. For the third series \(10 \times (6.5/6)^2= 17\) instead of 18. This implies that the first test of each series was evaluated independently of each other.
- 177.
Pars posterior, p. 387. Translation in [90].
- 178.
Pars posterior, pp. 394–395.
- 179.
Pars posterior, p. 394.
- 180.
Pars posterior, p. 396.
- 181.
Pars posterior, p. 397.
- 182.
pp. 47–48.
- 183.
Chapter 2.
- 184.
Proemio.
- 185.
Proemio.
- 186.
p. 431, first col.
- 187.
p. 1.
- 188.
Diffraction refers to various phenomena which occur when a wave (and light has the behavior of a wave) encounters an obstacle or a slit. It is defined as the bending of light around the corners of the obstacle or slit into the region of geometrical shadow. The term proposed by Grimaldi affirmed over the name inflection suggested by Newton in the title of his Opticks: or a treatise of the reflections, refractions, inflections and colours of light.
- 189.
p. 2, col. 2.
- 190.
For the experiment be successful the light intensity must be high otherwise the phenomena Grimaldi wanted to highlight may not occur.
- 191.
p. 2, cols 1–2.
- 192.
p. 3, cols 1–2.
- 193.
p. 3, cols 2.
- 194.
pp. 4–5.
- 195.
p. 9.
- 196.
pp. 13–14.
- 197.
p. 12.
- 198.
prop. 8, p. 104.
- 199.
p. 111, col. 1.
- 200.
p. 90.
- 201.
p. 18. cols. 1–2.
- 202.
p. 533, col. 2. For Grimaldi’s conception of the structure of matter see [86].
- 203.
vol. 2, pp. 102–103.
- 204.
p. 189, cols 1–2.
- 205.
p. 218.
- 206.
Preface. Not numbered pages, third page.
- 207.
pp. 352–399.
- 208.
p. 61.
- 209.
p. 82.
- 210.
p. 135.
- 211.
p. 9. Translation in [176].
- 212.
p. 6. Translation in [176].
- 213.
pp. 6–7.
- 214.
pp. 7–8.
- 215.
p. 8.
- 216.
Not numbered page near the end of the book; former proemio
- 217.
Table of contents.
- 218.
pp. 95–104.
- 219.
p. 48.
- 220.
In [176], p. 141, it is stressed that 3000 Florentine braccia equal 5925 English feet, or about 1.8 Km.
- 221.
p. 158.
- 222.
p. 163.
- 223.
p. 25.
- 224.
vol. 1, p. 3.
- 225.
p. 15.
- 226.
p. 29.
- 227.
vol. 10, p. 239; 228–229.
- 228.
p. 59.
- 229.
pp. 1–2.
- 230.
pp. 60–61.
- 231.
p. 65.
- 232.
p. 2415.
- 233.
p. 3.
- 234.
pp. 277–450.
- 235.
p. 76, and related footnotes.
- 236.
p. 182.
- 237.
Preface.
- 238.
p. 12.
- 239.
pp. 1–2.
- 240.
p. 1.
- 241.
p. 4.
- 242.
p. 7.
- 243.
p. 199–200.
- 244.
p. 17.
- 245.
Using the modern categories of mechanics, if x is the elongation of the spring of stiffness k and v the speed of a body having mass m appended at one end of the spring, the following relation holds good \(1/mx^2+1/2mv^2= 1/2k\text {X}^2\), with X the maximum elongation of the spring (associated to a vanishing speed) – principle of conservation of mechanical energy. From this relations one can obtain \(v^2= k/m (\text {X}^2-x^2) \propto (\text {X}^2-x^2)\). But \((\text {X}^2-x^2)\), with \(X=\text {AC}\) and \(x=\text {AB}\), is proportional to the areas of the trapezoid BCDE, thus if Hooke for speed intended the value at B, his conclusion is correct.
- 246.
p. 18.
- 247.
Area \(\text {BCDE} = 1/2 (\text {AC} \times \text {CD} - \text {AB} \times \text {BE}) = 1/2 \tan \widehat{\text {CAD}}(\text {AC}^2-\text {AB}^2) \propto (\text {AC}^2-\text {AB}^2)\).
- 248.
This statements can be justified when admitting direct proportionality of time (t) [B\(_i\)I] ] to space (y) [CB\(_i\)] and inverse proportionality of time (t) to speed (v) [B\(_i\)G]. This is in general only valid for uniform motion, but Hooke ignored this limitation, assuming v as a mean value. From the given proportionality between t, y, v, using a modern notation, one can write, \(y : v=t\), or equivalently \(v : \sqrt{y} = \sqrt{y} : t\), that is the relation proposed by Hooke , considering that \(v = \text {B}_i\text {G}\), \(y = \text {CB}_i\) and \(\sqrt{\text {CB}_i}=\text {B}_i \text {H}\), by construction. The cumbersome procedure allows to obtain [B\(_i\)I] by means of a geometrical construction.
- 249.
p. 130.
- 250.
p. 330.
- 251.
p. 330.
- 252.
p. 331.
- 253.
p. 331.
- 254.
p. 118.
- 255.
pp. 288–289.
- 256.
pp. 341–342.
- 257.
p. 17.
- 258.
vol. 5, pp. 281–291.
- 259.
Experiment 1, p. 12.
- 260.
Experiment 20, p. 71.
- 261.
To the reader; second not numbered page.
- 262.
pp. 59–60.
- 263.
Notice that Walter Charleton (1619–1707) in his Phisiologia of 1654 used the term molecule to indicate aggregates of atoms, or first convention of atoms [53], p. 109.
- 264.
vol. 1, pp. 524–525.
- 265.
vol. 1, p. 308.
- 266.
vol. 1, pp. 298–457.
- 267.
pp. 574–576.
- 268.
p. 26.
- 269.
p. 43.
- 270.
vol.3, p. 426.
- 271.
vol. 1, p. 4.
- 272.
p. 112.
- 273.
The contents; modernized.
- 274.
Marin Getaldić (1568-1626). A Dalmatian mathematician and physicist who studied in Italy, England and Belgium. He was one of the few students of François Viète.
- 275.
Preface.
- 276.
pp. 4–7.
- 277.
pp. 8–15.
- 278.
pp. 26–31.
- 279.
p. 117. Only a part of the proposition of paradox VI is referred to; there is a second less essential part which is ignored.
- 280.
p. 488. Boyle figure (Fig. 5.28) is identical to that of Stevin.
- 281.
pp. 121–123. Boyle said that Stevin’s proof may fail of mathematical exactness [39], p. 120, and that the “learned Stevin us, having demonstrated the proposition, because of some conjectures of which the truth had been more questionable than the theorem itself” added an appendix with some “pragmatic examples” to better justify the paradox [39], p. 135. Boyle underlined that hardly Stevin had experimented them.
- 282.
p. 499.
- 283.
pp. 137–139.
- 284.
pp. 140–141.
- 285.
vol. 10, pp. 69–79.
- 286.
p. 464.
- 287.
vol.1, pp. 1–185.
- 288.
vol.1, pp. 118–185.
- 289.
vol.1, pp. 186–242.
- 290.
vol. 1, Experiment 36, p. 86.
- 291.
vol.1, Experiment 4, p. 18.
- 292.
vol.1, Experiment 1, p. 11.
- 293.
p. 493.
- 294.
A defense of the doctrine touching the spring and weight of the air, Chap. V.
- 295.
The values e of columns E are obtained according a relation that with a modern language reads: \( e=\frac{48}{a} \times 29 \frac{2}{16} \) where a is the value indicated in the first column A. Notice however that because Boyle has not the modern concept of pressure, intended as force per unit of surface. his pressure is simply a force. So most probably Boyle would not understood the modern formulation of his law.
- 296.
vol. 1, pp. 156–160.
- 297.
An examen of the greatest part of Mr. Hobbs’ dialogus physicus de natura aeris, p. 59 [297]
- 298.
pp. 148–182.
- 299.
p. 152. Translation in [122].
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Capecchi, D. (2018). Post-Galilean Epistemology. Experimental Physico-Mathematica. In: The Path to Post-Galilean Epistemology. History of Mechanism and Machine Science, vol 34. Springer, Cham. https://doi.org/10.1007/978-3-319-58310-5_5
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