Vincenzo Galilei and Musical Experiments
Definition
1. Introduction
2. Empiricist Instances in Galilei. The Dialogo della Musica Antica et della Moderna
Judicious and learned people are not content as the inexpert multitude is with the simple pleasure of viewing colors and diverse forms of objects, but with investigating afterwards the agreement and proportion of its elements and its properties and nature.
I wish in those things which sensation can reach that authority always be set aside (as Aristotle says in the Eighth Book of the Physics), and with it the tainted reason that contradicts any [sense] perception at all of truth. For it seems to me that those who for the sake of proving some conclusion of theirs want us to believe them purely on the basis of authority without adducing any further arguments are doing something ridiculous, not to say (with the Philosopher) acting like silly fools.
The geometer makes no use of the faculty of perception: he does not train his eyesight to assess the straight or the circular or anything else of that kind either well or badly: it is rather the carpenter, the wood-turner, and some of the other crafts that concern themselves with this. But for the student of music accuracy of perception stands just about first in order of importance, since if he perceives badly it is impossible for him to give a good account of the things which he does not perceive at all.[16] (pp. 150–151)
In this sense we can tell, by way of example, the ratio of the diapason through lines; and through them, as if born of them, the diapason may be said to lie between the half and the whole, or, if we wish, the one and the two. However, these must not be considered simply as cardinal numbers [numeri numerati], but as numbers measuring only those portions of the strings capable, when struck, of producing a pitch. For what Zarlino says in chapter of the first [book] of the Istitutioni, maintaining that number is sonorous, cannot stand in any case, for, not having in itself body—and sound is not produced without the percussion of some body capable of rendering a sound—a simple number, consequently, cannot be sonorous.
Alongside the former, we can also include the Musici de Vulgari, who have a true understanding of practical music. They form and fill major and minor intervals using a variety of strings and accommodate them in accordance with the principles of counterpoint. As a result, when moving successively from one consonance to another, the ear, as I said of the eye, can desire nothing more. However, they are not familiar with the art of making music in a way that calms the intellect by expressing concepts through sound and voice, or inducing affection in others. Many of them firmly believe that they have found, known and perfected this art, but experience shows us that this is not true. Many of them would be able to put this belief into practice if they knew it, and they should be excused since until now they have had no insight into this matter, only much darkness and confusion of errors. They will not be able to excuse themselves in the future since it is clearly demonstrated to them that the purpose of true music is not what they have believed until now, but rather the purpose of false music.[20] (p. 105)
I find through long observation that natural voices and instruments made by art do not actually play or sing in this modern music practice any of the nine ancient diatonic species in their simplicity. Our practicing contemporaries inadvertently use only three of them today, mixed together in different ways. These are the intense [diatonic] of Aristoxenus, the ancient ditonic diatonic, and the diatonic syntonic of Ptolemy [authors’ note: Aristoxenus’s intense diatonic genus divides the tetrachord into five equal semitones, the ancient ditonic diatonic genus (i.e., the Pythagorean one) divides the tetrachord into two equal tones and a limma, the diatonic syntonic of Ptolemy correspond to the just intonation [21] (p. 22)]. Among stringed instruments, I consider that the viola d’arco, the lute, and the stringed fretted lyre play the intense diatonic of Aristoxenus. Hearing and seeing in these instruments the uniformity of tones equally divided into two identical semitones impels me to believe that this is true, for the aforementioned intense diatonic of Aristoxenus was distributed in such a way, as you will understand in due course. However, the organ, the gravicymbalo, and the modern harp [...] in the division of tones, for example, the tones are separated into two unequal semitones. The wind instruments like direct flutes, transverse flutes, cornets, and other similar ones have power, due to the distribution of their holes and aided by the fine facility of their wise, expert players, to adjust to one [species) or another according to the need and their [player’s] wishes. This is equally true of voices, but only when they are not willing to go against their nature and adapt to those [species]. Moreover, concerning the composing and singing of today, I am persuaded, because of what I told you and am about to tell you, that the ditonic diatonic is mixed with the syntonic of Ptolemy.
The Role of Girolamo Mei
3. Discorso Intorno all’Opere di Messer Gioseffo Zarlino da Chioggia and Scientific Papers
I wish to draw attention to two false opinions born among men, persuaded by the writings of some. I, too, had been among those. About these opinions, inasmuch as I am finally assured by means of experience, the master of things, I say this. They believe that the weights that Pythagoras attached to the strings in order to better hear the consonances were the same as those of the hammers from which he first heard them. Now, that this neither was nor could in some fashion be, experience (as I have said) demonstrates to us because one who wished to hear the diapason from two strings of equal length, thickness, and purity would of necessary suspend weights that were not in duple proportion (as were the hammers) but in quadruple. The diapente will be heard whenever weights of duple sesquiquarta [9:4] proportion are suspended from the same strings [...]. It is not true, therefore (and this is the other abuse), that the consonances cannot be had from other genera of proportions than the multiple and the superparticular.[...]Equally, we will have the diapason from pipes whenever the length and the void—or we might wish to say the diameter—of the low pipe is double the higher pipe. We will have the diapente from those where the diameter and the length are sesquialtera; and the diatessaron from those where their diameter and length be sesquitertia.
So, the void of these pipes corresponds to the cube; the weights suspended from the strings correspond to the surfaces; and the strings simply stretched on the instrument correspond to the line.
3.1. The Role of Experience
- 1.
- Ordinary experience was essentially static in nature, resulting from relatively simple items of information layered throughout the history of the members of a given society. In contrast, critical experience, especially at the beginning of the early science, was dynamic in nature, meaning it was constantly evolving.
- 2.
- Ordinary experience was based on authority and might also contain untrue statements, reported in written texts containing extravagant information, such as the claim that people from certain regions have two heads. Critical experiences involves gathering the testimonies of observers interested in reporting the facts as they have observed them.
Galilei’s Experiments
I am now coming to say with greater strength, that the fifth in the 3:2 proportion is the most perfect, sweeter than it is in any other ratio, as I have judged by ear after many many experiences [sperienze] (for I know no better means for attaining certitude).
The fifth, within the sesquialtera, not only seems to possess, but actually does possess a small degree of hardness due to the extreme amount it can be augmented, which avoids my saying (together with others of delicate hearing) that it is harsh. In the manner of Aristoxenus, however, it seems that the small degree of diminution gives it grace and causes it to become more in keeping with the taste of today, that is, soft and languid, and I do not believe that that happens for any other reason except being accustomed to hearing them continually under that form, or a similar one.
For among coins of the same goodness of material, of the same weight, cavity, thickness, and height, and also among little copper bells poured from the same mold, I have often found a difference of a whole tone.
We cannot have any means of modulating from a low to a high pitch and from high to low through continuous quantity except by tightening or relaxing a string without stopping it with the finger; or from a glass vase by raising or decreasing the level of water while revolving the finger on the surface of the rim of this vase or glass, however you want to call it. In these modes the ear also, because of its imperfection, judges the effect in the same way that we said it judges the stopping of a string on the fingerboard of a viola.
- 1.
- Direct and empirical, according to which, for example, two strings are in unison when they produce two sounds of the same pitch.
- 2.
- Indirect and mechanical, according to which two strings are in unison when they are of the same material, length, diameter, and tension [21] (p. 104).
It is possible to stretch to a unison two strings of the same material, length, and goodness, but if the thickness is different, their sound will depart from a true unison to the extent that there is an inequality. When the sound of these strings reaches the hearing-at least that of persons versed in such matters-the hearing will recognize an audible difference.
Now I shall ask those [who believe it is possible to tune in unison] whether they detect any difference in their sounds when playing a string of copper or steel and then or at the same time one of gut of the same thickness, length, and goodness in unison with the first and fulfilling whatever other conditions according to their method. If they answer truthfully, they will say yes.
They reply that, given any two strings stretched to a particular tension, I can raise or lower the pitch of one more or less than the other. I answer yes, and they reply that, since I can raise or lower one more than the other as I wish, I can make them equal and unisonant. In this case I reply as Aristotle did to those who denied the squaring of the circle, for they responded just as do the people I am talking about. Aristotle says, then, that since you can find a circle greater than a [particular] square and another smaller than that square, you can consequently find one that is precisely the size of the [required] square. I do not deny that this can happen, but I say as well that this circle equal to a square has been sought by the greatest intellect this world has known as long as the world has existed, yet it has not been found, so far as I know.
If I place on a lute one gut string and one steel string and stretch them to be in unison in their way; then if, for example, I position seven frets and I pluck the open strings, or if I position twelve frets (and then pluck the open strings), they will not be in unison [...]. The same happens to the ear as happens to the sight when two lines are so close to being parallel that in the space of a hundred paces they depart only by a fourth of an arm’s length. This difference divided by one hundred is so minimal that it would not be detectable by the sense, nor would the sense discern it in the space of a single pace, but in one hundred, yes.
I now ask them whether a song sung with discretion by men of judgment, acute hearing, and good vocal disposition would not be better than when played by some excellent player on an instrument tempered according to the intense tuning of Aristoxenus.
They will reply after hearing it sung and played that it satisfies them more played than sung. And they will speak correctly for reasons I will give now. Voices, being naturally perfect, when well developed4 by the art of singing, cannot sing well a song that is not composed according to their perfect usage, but an instrument tempered according to the imperfect usage in which this song is imperfectly composed, on the other hand, can play it.
3.2. Experiments on Vibrating Strings
The second way of hearing the same diapason, which I said by way of example was through surfaces, is between two strings made of the same material, equal in length, thickness, and goodness from which weights are hung related to each other not as the duple [ratio], as some have said, but in quadruple proportion. From the sound of these strings when they are struck at the same time a diapason will be heard.
The same thing will happen if equal weights are suspended from two strings the thicknesses of which are in quadruple proportion, provided the length and goodness are the same.
I believe that it [the diapason] may be obtained through other terms and through other means, as by striking rods, vases, copper and silver coins, and other things. But these will be vague and not the determinate weight, size, and number demonstrable with strings and pipes. For among coins of the same goodness of material, of the same weight, cavity, thickness, and height, and also among little copper bells poured from the same mold, I have often found a difference of a whole tone [emphasis added].
This same variety of the ratios of the diapason may be found also among strings of the same material, equality of length, and goodness, but of uneven thickness, when the same quantity of weight is suspended, and in other ways that I have experimented with many times [emphasis added].
Mersenne Law
- 1.
- The pitch of a string made of a given material, with a given cross-section and tension, goes down by an octave when its length is doubled.
- 2.
- The pitch of a string made of a given material, with a given cross-section and length, rises by an octave when its tensile stress is quadrupled.
- 3.
- The pitch of a string made of a given material, with a given length and tensile stress, goes down by an octave when its section is quadrupled.
- 3. The pitch of a string with a given length and tensile stress, goes down by an octave when its weight for unity length is quadrupled.
Here note that the heaviness of the moveable is more resistant to speed than is its thickness, contrary to what one might at first suppose, since it seems reasonable that speed should be more retarded by the resistance of the medium to being separated by a thick but light moveable than by a heavy and thin one; yet in this instance, the contrary happens.
3.3. Behavior of Organ Pipes
It is evident that Galilei did not do any experiments, since the pitch of a pipe is a function of its length and not of its cubic capacity. In his unpublished Discorso intorno alla diversità delle forme del diapason, he asks the question: what interval would be given by two pipes of the same diameter but one of which is double the length of the other? and answers that it could be an equally tempered major third.[32] (p. 24)
4. Conclusions
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Conflicts of Interest
Appendix A. Lute Strings in the Renaissance
Appendix B. Table of Galilei’s Main Musical Experiments
| 1 | Modern music practice as a matter of fact does not play as the ancient diatonic species | [12], p. 20 |
| 2 | Pipes correspond to the cube, weights to the square, and lengths to the line | [26], p. 20 |
| 3 | Comparison of the various consonances with the just fifth | [26], p. 117 |
| 4 | Rising the finger of the surface of the rim of a glass with different levels of water | [18], f. 54v |
| 5 | Observing the different colors of unisons from strings with different thicknesses | [29], f. 56v |
| 6 | Impossibility of a perfect unison | [29], ff. 59r–59v |
| 7 | Comparison of the same song sung by a good singer and an excellent player of an equally tempered instrument | [29], f. 61r |
| 8 | The octave can be obtained by striking rods, vases and coins | [18], f. 46v |
| 9 | In strings of the same length and tension the octave is obtained with thicknesses which are in quadruple proportion | [18], f. 46v |
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Capecchi, D.; Capecchi, G. Vincenzo Galilei and Musical Experiments. Encyclopedia 2026, 6, 68. https://doi.org/10.3390/encyclopedia6030068
Capecchi D, Capecchi G. Vincenzo Galilei and Musical Experiments. Encyclopedia. 2026; 6(3):68. https://doi.org/10.3390/encyclopedia6030068
Chicago/Turabian StyleCapecchi, Danilo, and Giulia Capecchi. 2026. "Vincenzo Galilei and Musical Experiments" Encyclopedia 6, no. 3: 68. https://doi.org/10.3390/encyclopedia6030068
APA StyleCapecchi, D., & Capecchi, G. (2026). Vincenzo Galilei and Musical Experiments. Encyclopedia, 6(3), 68. https://doi.org/10.3390/encyclopedia6030068

