by Mimmo Peruffo
- Picture nr. 1 to 18 : 17th-18th C string set ups: the diameter's progression seem to be far from an equal tension profile
- Picture nr. 19-20 : 4th hole measurement made on the Charles IX Andrea Amati's viol (1570 ca?); maximum crossing diameter: 2.30 mm .
- Picture nr. 21-22 : Viola da Braccio with an "equal feel" setup.
The choice of the tension profile of a set up for bowed instrument for historical repertoires raises a number of doubts all concerning two fundamental questions:
a) what I choose will be historically correct?
b) is it going to cause problems of instrumental technique and / or quality performance?
Questions like these are by no means negligible, especially considering that the answer refers to a subject,- the survey on string setup for hystorical instruments -which is relatively young and therefore subject to potential and continous updating.
A careful reading of already known historical sources and of those more recently discovered, the contemporary rediscovery of the French and Italian historical method to manufacture gut strings (method that produces results substantially different from those obtained following the modern techniques that are aimed, above all, to produce stiff modern harp strings, for tennis or for surgery) is allowing to fill, step by step, what until a few years ago was essentially an uncertain jigsaw puzzle full of gaps.
Is it possible nowadays to provide a convincing picture of the tension profile at different historical periods?
We shall first define some terms:
- Equal tension: the diameter of the strings of a set up is calculated all at the same value of tension, expressed in Kg
- Equal tactile sensation of tension (feel): the strings, pressed one by one at the same distance from the bridge (and in a state of intonation) express the same sensation of tactile "hardness" .
- Scaled or degrading tension: going from first thin string and passing to thicker strings they are calculated so that the tension is gradually decreasing.
Tension profiles of a Violin set-up
Equal feel and equal working tension
It is widely known that the rule to follow in set up for bowed instruments for repertoire of the sixteenth and seventeenth century is the one that leads to a profile in equal tension between the strings. (1) (2)
If we observe it more in detail, we will come to a different result.
It should be clarified first three basic elements:
1) In the seventeenth century treaties and methods that deal with music and / or musical instruments, tension is almost never expressed by a unit of measurement, the term used is what leads us to consider rather the 'tactile sensation' of tension. This, as it is stated on the same treaties, must be equal between all the strings of the set up ('equal feel'). From a hystorical point of view, the first document of our knowledge, in which the tension of each string (in this case of the Violin) is expressed in Kg dates only 1869. (3)
2) A second element to be rememberd concerns the relative importance that has a speculative document compared to other sources that report information obtained, instead, from stringmakers of that time or concerning methods for musical instruments such as lute, etc. We believe that daily practice is better described in these methods or by construction data of string makers than in scarcely accessible contemporary disquisitions focused only on theoretical speculation. It is the same even today: in most cases are indeed string makers that push market towards the use of certain gauges and certain tension profiles instead of others.
3) There is a third element: the treaties of the seventeenth and eighteenth centuries can easily lead to ambiguous situations. A typical example that brings to confusion between the equal tactile sensation of tension of the strings with the equal working tension is for example the following abstract from the Galeazzi: "
"la tensione dev'esser per tutte quattro le corde la stessa, perchĂ¨ se lâuna fosse piĂš dell'altra tesa, ciĂ˛ produrrebbe sotto le dita, e sotto 1'arco una notabile diseguaglianza, che molto pregiudicherebbe all'eguaglianza della voceâ".
('the tension must be the same for all four strings, because if one were more tense than another, that would create under the fingers, and under the bow, a considerable inequality very prejudicial to the equality of tone') (4)
By reading this passage with more attention is clear however that the 'equal tension' is actually referring to the feel of tension that you feel under the fingers or under the bow. Here's another one potentially misleading:
""Quanto una corda Ă¨ piu vicina al principio della sua tensione, tanto ivi e piu tesa. [...] Consideriamo hora una qualunque corda d' un liuto: ella ha due principj di tensione ugualissimi nella potenza, e sono i bischieri dallâun capo, e '1 ponticello dal1'altro; adunque per lo sopradetto, ella Ă¨ tanto piu tesa, quanto piu lor s'avvicina: e per conseguente, e men tesa nel mezzo".
('The closer a string is to the beginning of its tension, the tenser it is. [...] Just consider any lute string. It has two beginnings of tension that are absolutely equal in power: the pegs at one end, the bridge at the other. As a result, it will be tenser the nearer it is to those points and less tense in the middle') (5)
The concept of more or less tension is certainly related to a tactile sensation of tension and not to a real tension in Kg which, under static tension conditions of the string is obviously the same at any point on the string. From a tactile point of view it is more âstrenghtenedâ to touch as far as you move towards the fix-ends.
The evaluation criteria of tension: the case of Lute
The evaluation method of the string tension by finger pressure (or more exactly by right thumb) that tests their 'hardness' near the bridge was the universal criterion used for balancing set up of Lute Strings:
-John Dowland ('Variety of Lute Lessons', by Robert Dowland, 1610):
"Of setting the right sizes of strings upon the lute. [...] But to our purpose: these double bases likewise must neither be stretched too hard, nor too weake, but that they may according to your feeling in striking with your thombe and finger equally counterpoyse the trebles".
-Mary Burwell Lute Tutor (1670 ca.):
"When you stroke all the stringes with your thumbe you must feel an even stiffnes which proceeds from the size of the stringes".
-Thomas Mace ('Musick's Monument', London 1676):
:âAnother general observation must be this, which indeed is the chiefest; viz. that what siz'd lute soever, you are to string, you must so suit your strings, as (in the tuning you intend to set it at) the strings may all stand, at a proportionable, and even stiffness, otherwise there will arise two great inconveniences; the one to the perfomer, the other to the auditor. And here note, that when we say, a lute is not equally strung, it is, when some strings are stiff, and some slack".
From these statements results the following
1) the criterion for selection of the diameters of strings of a lute set up was carried out according to criteria of empiricism: the strings should not present too stiff or too slack but with a subjective right degree of tension feel.
2) that 'right' feel of tension should be the same across all the strings of the set up. If this does not happen then a serious mistake occurs.
It goes without saying that the judgement on the degree of tension can only be subjective. It is instead different the appearance of homogeneity of tension among the strings, which represents the true common criterion of lute players of the past.
We now are going to analyze in depth the issue of the tactile feel of tension.
The tactile feel of tension
When a string is moved laterally by means of a pressure practised on it (by means of fingers, bow etc) it carries against the pressing element an equal and opposite action with the aim to counteract that pressure.
Such contrast, for a particular value of lateral shift, is going to produce a certain feel of effort on the part of the one who puts pressure on the string.
We talk about equal feel, when with the same lateral displacement, the sense of effort is the same even between strings of different type, diameter, etc., provided, however, that the point of pressure is always the same.
Trying to bring in scientific terms the notions of even stiffness, equally strung etc. described in the seventeenth century treaties like those above cited is something complex in itself, both because there is no evidence to confirm that they all intended the same by âfeelâ and because the so-called feel can also be understood in a âbroaderâ way.
There is meanwhile a first distinction to be made: whether to press the strings to evaluate the degree of 'tension' are directly the fingers of right hand or the bow. (9)
In the second case thicker strings (and therefore with more surface area in contact with horsehair), even if at the same working tension of thinner ones, can put up a higher resistance to friction thus making the player the feeling of a certain higher 'tension'.
In the likely hypothesis that the fingers and not the bow (as evidenced by the fact that treaties of the seventeenth century are practically always related to the lute) aimed to understand how stretched the strings are, we can understand the feel in at least two different ways:
The first one (commonly accepted and supported also by us): it considers the effort that must be done with a finger (usually the right hand thumb) to move laterally (usually downward) to a certain extent a string. This string will obviously create a resistance against the pressure. By substituting the finger with a weight acting at the same point, it can accurately be measured the extent of lateral shift for each string examined. The feel will therefore be the same, when the lateral displacement will be the same for all strings tested.
The second one: it considers that the thinner string, sinking further into the tip of the finger that presses it, would produce a higher feel of tension of a bigger string, which having a larger surface does not sink in the finger in the same way. (10)
According to this second interpretation an equal feel requires a higher working tension in the thicker strings than in thin ones. However, there is no evidence that bass strings presented a tension in Kg higher than the trebles. There is evidence to the contrary, if anything.
We now investigate the first hypothesis, that namely considers as feel the sensation of resistance made by a string pressed by fingers, not considering its diameter, and as 'equal feel' the fact that the opposing force is the same (with the same displacement caused by acting finger) even for strings of different gauges or different manufacturing technology put into traction.
Physics has shown, by calculation, that equal feel as stated above corresponds exactly to an equal tension set up
But here comes something that has not been revealed so far: equal feel do correspond to an equal tension but under condition that the strings are already in a state of traction.
But this condition has nothing to do with the common practice where the diameters of the strings of the set up in 'equal tension' are obtained directly by mathematics calculation. In this way, the diameters are in fact those of the strings âpackaged â, i.e. at rest.
The difference between the two conditions is crucial: a string already in a state of tension is a string that has been subject to some stretching, then has no longer the diameter that had been calculated, but smaller.
In order to achieve the condition equal feel = equal tension in Kg, the strings should therefore keep unchanged their diameters even after being brought to tuning or at least that all gauges are reduced according to same percentage.
In practice (and this is evident in the gut more than in other rigid materials ), this does not happen: once the strings are brought into traction, each of them will reduce its diameter to a certain percentage which is a function of the position in the instrument (in other words related toÂ the Working Index ) and how the string was made.
The Working Index is the parameter indicating the fraction of tensile strength used by the string compared to its maximum strength. This value derives from vibrating length multiplied for the frequency of the string. Its maximum value coincides with the breaking stress and is a function, as mentioned before, of construction parameters such as the amount of twist, the kind of twist used (similar to nautical line, high or low twist, etc.), quality of raw material, the use of specific chemicals which may contribute in increasing or reducing it, etc.. It goes without saying that the higher the working tension, the greater the strengthening of the string.
The tensile stress is highest for chantarelles (the Lute trebles exploit as much as 91-95% of their total available reservoir of tensile strength, which means that they undergo, among all, the greatest stretching under tension) and so on in smaller percentage on bass strings positions (lower Working Index). But this is not because the trebles are thinner but because their Working Index (the product of frequency and string length) is the highest among those of each string of the set up.
The explanation is simple: in a larger string the same tension is âspreadâ in a bigger section than a thinner string. Consequently, the applied tension-referred to single section will be lower. Hence a lower stretch of the string. A thicker string, in other words, is considered as composed by many theoric thin strings stuck together to make the diameter required. It is obvious that if full tension is applied to one of these hypothetical thin strings it will become much longer (it is the case of thin treble) but if the same tension is instead spread among this theoretical quantity of thin strings, here so that each of them shall be subject only to a fraction of the total tension thus producing a lower final stretch.
Between two strings of different diameter, constructed in the same manner and subject to the same tension, the thinner one will stretch much more than thicker one because of largest load insisting on the cross section. On gut strings in particular, longitudinal lowering is divided into recoverable lowering and not recoverable one, in practice a new string that has undergone initial tensioning, when placed to rest does not recover completely as the starting length. As the string stretches due to increasing stress (the difference will wrap around the peg) its diameter will gradually reduce. Well, the reduction in diameter will also result in a simultaneous decrease in operating tension (tension and diameter are indeed directly proportional)
As mentioned above, the strings that occupy the position of treble (because of higher traction per unit cross section) are those that decrease in a higher percentage than the others and so progression as we move to bigger ones (it is well known that in a violin many more turns of the peg for treble strings are required than for third string).
It follows therefore that their working tensions (which were formulated at the beginning from theoretical calculations as identical), in the final state of tune will no longer be equal but will take a new structure which will now be scalar: the treble strings will be, among all, the ones that will have the lowest working tension.
But if the string tension in a state of tone is different, here then also the 'feel' between the strings will no longer be the same. It will consequently have not a homogeneous tactile profile but a scaling one: the treble will be softer to the touch while the lower strings will need a greater pressure from the fingers.
At this point the equation equal feel = equal tension is no longer valid.
Conclusion: a set up in equal tension cannot be considered a historical set up: we would like to stress once again that the treaties of the seventeenth century for lute do condemn fairly clear a set up in case it has a non homogeneous feel. (Op. cit 8)
Using a violin (but it would be fine also a guitar or a lute), we tested two gut strings calculated to have both the same tension (8.3 Kg pitch of 440 Hz) at required tuning ('E and D in our case). The string length is of course the same for both (33 cm).
The diameters we use are as follows: .65 mm for the 'E' and 1.45 mm for the 'D' measured 'in rest', i.e. not in tension. The thinnest string had a so-called 'medium' twist (45 Â° approximately) while the thicker was 'high' twist. (<60 Â°).
Once tuned and stabilized we proceeded to verify by micrometer their diameters: E gauge dropped to .62 mm, while for D we did not find an instrumentally valuable decrease. The thin string has therefore experienced a reduction in diameter of 5% (.62 / .65 mm). While D string it was considered virtually unchanged (<0.1%), despite its degree of twist (and elasticity) is significantly higher than that of the treble.
It should be emphasized that these measures are derived from a single experimental test: strings manufactured differently than the samples examined by us may provide different percentages of reduction. In our case, the underlying tension of the strings on the instrument was reduced to 7.6 kg for the 'E' and 8.3 kg for the 'D' compared to the tension used for theoretical calculations and equal to 8.3 kg .
In order to have a 'E' and a 'G' in the state of tuning keep same kg then it will be necessary to increase the initial diameter of E only' (please note that the 'D' is virtually unchanged) of 5%.
In this state of tune then you are going to loose this âextraâ. In conclusion it will be required a diameter âpackagedâof .68 mm while the 'D' shall remain equal to 1.45 mm.
Deriving tensions in this second set of strings in the resting state, there is therefore a scaling tension: 9.2 Kg for the 'E' and 8.3 kg for the string 'D'.
Unfortunately it is not possible to determine by mathematical calculation of how much string will reduce its diameter under load, because this parameter is the result of several variables specific function of the system with which it was built, the only valid method, then, is the experimental way starting from a set up in which gauges are known, provided that the type of strings are the same.
The experiment shows that the gauges of .65 and 1.45 mm in equal tension, in a state of tuning will reconvert producing some scaled in the working tension and consequently a lack of homogeneity even in the tactile feel. Using instead a compensatory diameter of .68 mm and 1.45 mm (according to a 'resting' scaled tension profile) operating tensions will then re-set so as to finally bring the hoped equal tension, or same tactile sensation (i.e. equal feel).
If you wish a set up in equal feel according to the historical criterion it is therefore necessary to start with a choice of diameters of string âpackagedâ' calculated according to a scaling profile.
What we expressed so far, gives finally an explanation of the relationship between the feel and tension of work. It can be applied easily to the family of the lute and plucked instruments, but what about the string instruments?
Criteria in the historical set up of stringed instruments
With the exception of theoretical Serafino Di Colco (1692) (11), we do not know indeed any treaty of Sixth -Seventeenth century able to provide some explanation about the criteria used in daily practice at that time. In practice, today - and missing better ones â are applied the criteria established for the Lute (same feel, same tension). But are we sure that this operation is technically correct?
The Lute is a fact quite different from the stringed instruments:
1) it must be plucked and not played with a bow.
2) it has courses in unison and octave, and not of single strings.
3) working tension are significantly lower than those of bowed instruments
4) it has a fingerboard and a bridge that are flat and not arched
5) it is provided of frets that go to determine with some accuracy the frequency of notes played
Only one of these criteria - the frets -is shared with the family of Gambas, while are excluded the violin, the viola da braccio and the Violin Bass and some big Violoni.
Therefore, we analyse in detail the historical sources in our possession that relate in some way with stringed instruments:
The Sixteenth century
There is no document (other than of essentially speculative nature) dealing with the tension profile of a string instrument in the daily practice of contemporary musicians and of the area in which its author lived.
On the other hand, we have the dimensions of the holes of the strings of two viola da braccio present the Ashmolean Museum in Oxford (we know that these tools were re-necked). Our measurements made in year 2008 have shown that the tailpiece's hole for the fourth string, considered an original of Viola by Andrea Amati 'Charles IX' built around 1570 is 2.3 mm only: what explanation can we provide for this direct evidence?
Whereas in fact an hypotetica Venetian pitch of 465 Hz at vibrating length of 36 cm, with a diameter of string equal to 90% of the hole (2.1 mm approximately) for a fourth note âCâ you get a tension equal to 4,6 Kg only (range of working tension of a viola da braccio today in equal tension is around twice to close to 3.0 mm in diameter of string). In this period of history according to some researchers (op. cit. 2) had not yet come into use in the low string made like a rope, from acoustic point of view this makes things even more difficult.
The Seventeenth century
Mersenne (Harmonie Universelle, 1636) (12): the concept of equal tension arises as a theoretical principle where he explains the mathematical relationship between diameter, vibrating length, and density of the string and its working tension. Mersenne was indeed the first to put in relation these parameters and enunciating for the first time the law then called 'Mersenne / Tayler'.
But he took as a basis for its calculations only keyboard instruments (which are different from the strings, as far as the mechanical principle that leads to the production of sound is concerned).
In another well known example, he took the Lute as a model illustrating once again the inverse proportion between the diameter and the frequency (with the same tension and vibrating length and density of the material).
Mersenne in another chapter added sadly thatÂ very few,Â in his time was following in the daily practice what he explained. This is not a detail to be neglected, because it means that the equal tension was probably not a practice currently followed in everyday life of his time. (13)
Atthanasius Kircher (1650): In "Preludium 1" Kircher gives the number of fresh guts needed to produce the strings for Roman Violone â Est hic Romae Chelys maior, quĂ m Violone vulgĂ˛ vocant pentachorda, cuius maior chorda consesta est ex 200 intestinis. Secunda ex 180. Tertia ex 100. Quarta ex 50. Quinta denique ex 30. (14)
These data are very interesting as they set out in âdirectlyâ the number of guts to be used to make the strings of this great musical instrument, they were certainly given to Kircher by Roman string makers (Kircher indeed lived in Rome), who were the most active Europe.
Our goal is to check the tension profile so that is not important to know exactly the type of gut used, but only feel that all the strings have all been made from the same type of material. Assuming for example that with three whole sheep casing of about 8 months of age we get an average diameter of 0.70 mm, so by simple proportion it can be calculated as follows:
1: 2.21 mm (30 guts)
2: 2.85 mm (50 guts)
3: 4.04 mm (100 guts)
4: 5.42 mm (180 guts)
5: 5.71 mm (200 guts)
The author fortunately states how Chelys Maior is tuned : E treble, A, DD, low GG . The difference between the number of guts between fourth and fifth string can mean that there is only one interval of distance: so low FF
We calculate the tension considering a Roman pitch of 392 Hz and a fake vibrating length of 90 cm:
1: 35.50 kg for the first string E
2: 26.31 kg for the second string A
3: 23.54 kg for the third string D
4: 18.88 kg for the fourth string G
5: 16.64 kg for the fifth string F
As you can see the series of tensions of work leads to a scaled profile that probably also brings to an equal feel.
This figure can be considered direct evidence of the use of a scaled profile in the seventeenth century with data (the number of guts for each string) that refer directly to Roman string makers, i.e. at those who were certainly capable of imposing a certain line of conduct in the choice of commercially available diameters.
A final clarification: on page 486 of the Treaty there is a table on the strings of "Chelys exachorda" column II shows a series of numbers which do not indicate the diameter of string (which would remind a set up in equal tension) but the proportions between the frequencies of the strings played open (i.e. not fretted) . It is not a coincidence that the column is called 'propor'.
Serafino Di Colco (1692)
Di Colco wrote, âSiano da proporzionarsi ad un violino le corde [âŚ] distese, e distirate da pesi uguali [âŚ]. Se toccandole, Ă˛ suonandole con lâarco formeranno un violino benissimo accordato, saranno bene proporzionate, altrimenti converrĂ mutarle tante volte, sin tanto che lâaccordatura riesca di quinta due, per due, che appunto tale Ă¨ lâaccordatura del violinoâ. The researcher Patrizio Barbieri- believes - and we agree - that these considerations are purely speculative. (15).
However, is difficult to imagine that each musician has been provided with equipment such as that represented by him:
The case Di Colco can easily lead to some confusion of interpretation. In fact, we are tempted to conclude that are handled set up of equal tension according to modern practice, i.e. as if the diameters were derived from a calculation on strings âpackagedâ (not under traction).
But things are different: the test indicated by Di Colco takes place with scheme to ensure equal weights (i.e, a real equal tension), but in a completely different condition from equal tension as advocated today. Today equal tension derives the diameter of the string not under traction (the consequences of which have already been discussed above) while in the case of Di Colco strings are effectively already in a state of intonation, ie which have already undergone the process of stretching due the tension imposed by weights.
As it is a situation of equal dynamic tension (the weight remains the same even if the strings stretch)
strings show a condition not of equal tension according to the modern principle but of equal feel.
The method suggested by Di Colco realizes, in other words, what we mentioned above, following however a reverse path. It is obvious that the strings then found suitable for the purpose of tuning in fifths, would have shown diameters packaged that lead to a tension profile moderately scaled, exactly like the other cases described. Put in tension they will stretch up to in a diversified manner until arriving all at the same operating tension (given by the same activated weight).
Di Colco set up, in other words, is actually a set up that requires a starting choice of strings that according to current calculations leads to a moderately scaled tension profile which will then express the equal tactile feel (and therefore equal tension in the state of intonation).
It still remains unclear, as in the case of Mersenne, if the theory by Di Colco was also the daily practice of the musicians of his time. On this point, other historical sources in our possession do not show anything useful, unfortunately. It is difficult to think that musicians of his time have all been provided with a âgimmickâ like that used by Di Colco for his interesting demonstration.
The examination of the iconographic sources of the Sixteenth and Seventeenth centuries can provide valuable insights about the general profile of string gauges of the musical instruments represented, provided that they are made with certain criteria of 'truthful'.
Fortunately, in an equal tension profile, the difference in diameter between the first and last string is noticeably marked , so that is perceived to be easily 'visible'.
However, in the gallery of images that we show, most part of examples do deviate not only from what could refer to a profile of equal tension but, in some cases, that could draw to an equal feel:
Indeed the iconographic examples where you can find an interesting difference between the apparent diameter of the first string compared to lower strings are only a few:
Pictures in which the difference in diameter between the treble and the fourth string is more evident
Even though we are dealing with painted images and not photos, what can be seen in the iconography of Seventeenth century (especially on one that reserves a great deal of attention in the reproduction of reality) draws a picture in which the possible explanations are more in the direction of a scaled tension profile than of equal tension, moreover there is also the possibility that the low strings are represented so thin not only because of a particular profile of tension but perhaps also because some manufacturing aspects of the strings (loaded gut?).
The Eighteenth century
Some researchers believe that in the Eighteenth (and also in the early Nineteenth century) there was a coexistence of the profile in equal tension and the strongly scaled. This view in our opinion is not historically sustainable. (Op. cit. 2).
Towards the middle of the Eighteenth century was beginning to define in practice some of the characteristics of the set up for stringed instruments of the time (mostly related to Violin):
1) the tension -profile reported in the documentation is scaled
2) the degree of scaling does not match with the one deriving from equal feel; the slope in the tension is in fact higher:
We do not know the reasons why the violinists of the time took that choice, unless this aspect was already part of the daily practice of the Sixth-Seventeenth century (see the iconographic aspect of and the measures of the holes of the strings of the Viole Amati).
We cannot see any logic that could justify the abandonment of an eventual tactile equal feel profile to adopt a so scaled tension.
The adoption of wound strings indeed does not make this change necessary.
1) Handwritten recipe (probably early Eighteenth century): the number of guts suggested to make the top three strings of the violin leads to a very scaled tension profile (16).
2) De Lande (1765-6): he reported very interesting information on the activities of the most talented string makers in Abruzzo region (Italy) -Angelo and Domenico Antonio Angelucci-latter 's death in 1765 and that, in the first half of the Eighteenth century, had the most important works of strings of Naples, which numbered more than a hundred workers. In this document we learn that to make the first string of the violin they took three whole lamb intestines of eight to nine months of age, while for the last (ie last intending gut only, i.e. âDâ', which is certainly not the fourth, which as we will see later, was a wound string) they took seven. The fourth string was a wound string. (17)
3) Conte Riccati (1767) The Count makes no new theory in regard to the tension profile compared to the past as some scholars argue. (18) He introduced a simple mathematical explanation to justify the reason of the scaling of the string tension of the commonly available strings that he finds on his violin. The book of Riccati was started around 1740: so in commercial sense, therefore, the violin strings available on the Italian market in the first half of the Eighteenth century showed a tension profile remarkably scaled (p.130):
âColle bilancette dell'oro pesai tre porzioni egualmente lunghe piedi 1 Â˝ Veneziani delle tre corde del Violino, che si chiamano il tenore, il canto e il cantino. Tralasciai d'indagare il peso della corda piĂš grave; perchĂ¨ questa non Ă¨ come l'altre di sola minugia, ma suole circondarsi con un sottil filo di rameâ. (Using gold-weighing scales, I weighed three portions, each 1 Â˝ Venetian feet long, of the three violin strings, those called the tenore, canto and cantino. I omitted the weight of the lowest string, because unlike the others this is not of gut only, but is usually surrounded with a thin copper wire).
If you consider an averaged specific weight of the gut of 1,3 gr/cm3 results to be respect .70; .91; 1.10 mm of diameter for âeâ"; "a" and "d" respectively (19).
4) Donato Vincenti (1785): All data provided by this string maker in regard to the number of guts used to make the top three strings of the violin all lead to a very scaled tension profile. To be clear, the same kind as those mentioned by De Lalande. (20)
Let us now examine in detail some 18th C. sources which are considered equal tension profile evidence
1) Stradivari (early Eighteenth century): the hypothesis of a possible equal tension set up to the Stradivarius violin that he used to guide the type of string to use for its Theorbo Guitar born as a result of the traces shown on the figure marked with charcoal of the ' TheorboGuitar': next to one of these tracks is in fact wrote:âQuesta in cima deve essere una quarta da ViolinoâŚâ ( the upper string must be like a violin 4th) (Op cit 2)
The track referred to the fourth string of the violin is of rather remarkable thickness: this was therefore not just a gut setup but also in equal tension.
Our assumptions are different: in this template Stradivari makes very large and coarse marks even those that are inevitably very thin string, such as the first three courses in the keyboard or the intermediate strings.
The trace of a string which he refers in the cardboard shape has a thickness of 3, maybe 4 mm is a measure of second-or third-string of a doublebass. We do not want really to believe that this was really the true measure of the fourth string in pure gut violin. Instead, we think that Stradivari meant to indicate that the string to use in that position was to be a fourth string of violin (an instrument certainly much better known by string makers and musicians), with no aim to give in the track made with charcoal its real diameter.
We find it frankly without any foundation, the conclusion that the violin to which he was referring to, was in equal tension.
In conclusion it is not possible to determine anything about the profile of tension of that violin and we cannot conclude with certainty that it was set up only with gut strings Stradivari could in fact have wanted to suggest that for that theorbo guitar string it had to use the fourth violin wound string.
2) Tartini (1734): Fetis wrote that Tartini in 1734 found that the sum of the tensions of the four strings of his violin was of 63 pounds (op. cit 2). Apart from knowing how Tartini determined that value of tension (and if this data was then successfully converted into other units of measurement) it should be emphasized that the mere fact of being expressed in a single global value, this does not mean that we are witnessing the confirmation of a set up in equal tension. This same value can in fact also be obtained from the sum of completely different tensions. Through some tests we came to conclusion that we are perhaps in front of a scaled type set up
1. Being a violin we consider a vibrating length of 0.32 meters.
2. for standard âaâ we can assume a theoretical Venetian pitch of the Eighteenth century equal to 465 Hz
Hypothesis of equal tension:
Assuming that 63 pounds are actually equivalent to 31 kg following the hypothesis of equal tension would result in about 7.7 kg per string that would bring to the following sizes:
âeâ: .61 mm
âaâ: .92 mm
âdâ: 1.38 mm
âgâ: 2.06 mm (expressed in equivalent gut)
As you can see the treble has a diameter that is out of the calibration range which can be obtained with 3 or 4 lamb casings, that is, as we know, the typical constructive characteristic of that particular historical period. (Op. cit. 16, 19)
Starting instead from an average value of a supposed 'e' of .70 mm (obtained from 3 -4 whole lamb casings ...) with a set up still in equal tension it can be observed that things do not settle at all: it would have a total value of tension of about 42 Kg. Therefore this hypothesis is not plausible.
It should be emphasized how the sum of tensions of the three thinner strings only (about 30 kg) would be enough to nearly reach the value of tension indicated by Tartini for all four strings).
Hypothesis of scaled tension:
Starting with an average value of 'e' of 0.70-mm and using the sizes of 'a' and 'd' as found in the average historical sources close to him (Conte Riccati, De Lalande) leads to the following data :
âeâ: .70 mm (9.9 kg)
âaâ: .90 mm (7.3 kg)
âdâ: 1.16 mm (5.4 kg)
Total 22.6 kg
In order to reach the 31 kg set by Tartini you must have a wound âgâ string that produces about 6.5 kg of tension: this corresponds to plain gut string of 1.90 mm. Manufactuing such wound string as specified by Galeazzi (op. cit. 4) it is indeed in the required range and this would therefore confirm the hypothesis of scaled tension compared to equal tension.
3) Leopold Mozart (1756): Mozart (22) considers the same concepts of Di Colco. He suggests to bring equal weights to each pair of adjacent strings, and a change of the diameter (âaâ comped to trebleâeâ ) until we succeed in obtaining open fifths. We proceed in this manner with the third and apparently also with the fourth strings.
Our conclusions are therefore the same as those made with Di Colco, we are talking about a tension profile that if it is calculated in accordance with the current practice leads to a tension profile of tension (derived from calculation) moderately scaled, not to an equal tension according to the current concept. (Op. cit 1, 2)
Here now some Nineteenth century sources supposed with the equal tension profile
1) Fetis and Savart (1840 and 1856): both show the total value of the tension of the violin specifying better how the tension was divided between the treble and the other strings. If the strings were in equal tension, for what reason it was specified that the treble took 20-22 pounds and the rest of the strings up to a total of 80 pounds? It was enough to define a single value of tension. We lean to the conclusion of a scaled tension profile also as a result of the contemporaneous scholar Delezenne. (22) (23)
2) Delezenne (1853): first, he formulated the theoretical hypothesis of equal tension but when he had to deal with a dozen sets of strings present in the market given to him by luthier Lapaix he realized that all all of them followed a strong scaled tension profile . (24)
3) Maugini & Maigne / Savaresse (1869): The tension values indicated in the text for the four strings are unreliable, they are fully in contradiction with the number of guts necessary to procuce them, which leads instead to a scaled tension profile similar to all other examples.
It should be noticed of the text a mistake in calculation or typing : the treble has a working tension lower than the second string (7, 5 kg compared to 8.0 kg of âaâ'), probably the correct value is 8.5 kg.
After deriving it from an estimation of the diameters (and a vibrating length of 33 cm and a pitch of 415 Hz), relating to the same breaking tension for each string in the text, there is a fundamental inconsistency: the breaking index of gut is too low, out of any acceptable standard: 33-36 Kg/mm2 for âeâ (and this is fine) and only 21 Kg/mm2 for 'a' and 17-19 for Kg/mm2 ' d '. This makes it unreliable to draw any definitive conclusion in favour of equal tension. If we start instead from the number of guts in the text by string maker Savaresse (for a scaled tension profile) the breaking index are again fully reasonable. (Op. cit. 3)
4) Huggins (1883): After having calculated the diameters according to an equal tension profile he realized that they did not work as expected. Afterwards he understood the validity of commercial gauges with strongly scaled tension as those produced by string maker Ruffini in Naples. Afterwards Huggins argued that theoretic gauges in equal tension do not give open fifths as well as a satisfying acoustic performance and he made all his efforts to understand why this happened. (25)
What might be the explanation of so marked scaled tension?
Huggins considers two hypothesis : the first takes into account the pressure excerted by each individual string on soundboard .
He points out that in the condition of equal tension (but also in equal feel, we might add) the pressures in Kg exerted by the first three strings on the below soundboard are by no means equal, and this depending by the angle of the string on the bridge moving towards bigger ones that gradually becomes more acute. It is determined in this way a higher pressure on the soundboard. In order to obtain equal pressures acting on the table by each individual string it is therefore needed an additional scaling compared to the condition so far considered.
The second hypothesis considers the fact that the strings gradually that are thicker , in practice, are placed gradually at a greater distance from the keyboard: therefore the fact that the fingers of his left hand in a position of equal tension / equal feel should do an extra effort to press on the keyboard. Hence the reduction of tension in order to recover consistency in the feeling of the fingers of his left hand.
A third and final hypothesis that weighs in favor of a (marked) scaled profile in tension consists on aiming to the maximum possible uniformity of friction to horsehair bow, as advocated by Riccati already in the Eighteenth century and again later by the second half of Nineteenth century by Pleissiard (26):
Egli Ă¨ dâuopo premettere, che quantunque lâarco tocchi una maggior superficie nelle corde piĂš grosse, nulladimeno la sua azione Ă¨ costante, purchĂ¨ si usi pari forza a premer lâarco sopra le corde. Questa forza si distribuisce ugualmente a tutte le pasrti toccate, e quindi due particelle uguali in corde differenti soffrono pressioni in ragione inversa delle totali superficie combacciate dallâarco.â (Giordano Riccati âDelle CordeâŚâ op. cit, p. 129).
The examination of different historical and iconographic sources in our possession might possibly allow to draw a sufficiently clear criteria for choosing a set up for stringed instruments in the seventeenth, eighteenth and nineteenth century (as seen in everyday practice, and not at the level of pure theoretical disquisition). If you cannot say with certainty which were the criteria used in the Seventeenth century , we can emphasize with some certainty which ones were not.
In first place there is the concept of equal tension 'by calculating' so prevalent today: despite the writings of Mersenne, seems not having been followed as common practice in the Seventeenth century.
Moreover, equal tension 'derived from calculation' unfortunately, is based on an error of scientific evaluation of the proper relationship equal tension= equal feel. The tension of this equivalence is that the string which is already tuned, not the one you set by the known formula for the calculation of the diameters.
It must be emphasized that this criterion of equal feel is still derived from the treaties for plucked instruments only like the lute and not for stringed instruments, for which we do not have actually anything really exhaustive. The first useful practical information date back only to the late Eighteenth century.
Our point of view, summarizing the existing corpus of information examined, aims to suggest in practice a scaled -type tension for most of stringed instruments: Kircher, moreover provides a real test. To determine how scaled it could be is unfortunately impossible to determine. It remains an open question on the open Fifths of fingerboard, which was for some researchers of the Nineteenth century, a topic to explain the need of scaled tension in stringed instruments. But if the problem of having the fifth in tune in the Nineteenth century was a real problemÂ (27), was it a problem even in the Seventeenth century?
Mimmo Peruffo 2010
1) OLIVER WEBBER: âRethinking Gut strings: a Guide for Players of Baroque Instrumentsâ. Ed: Kingâs Musik. London, 2006.
2) EPHRAIM SEGERMAN: "Strings thorough the ages", The Strad, part 1, January 1988, pp.54-55".
3) MAUGIN - MAIGNE: Nouveau manuel complet du luthier, pp. 168-181 (the string's section was added in the 1869 edition).
4) FRANCESCO GALEAZZI: âElementi teorico-pratici di musica con un saggio sopra lâarte di suonare il violinoâ, Pilucchi Cracas, Roma 1791, p. 72.
5) DANIELLO BARTOLI: Del suono, de' tremori armonici e dell'udito, a spese di NicolĂ˛ Angelo Tinassi, Roma 1679, p. 157.
6) JOHN DOWLAND: "Other necessary observations belonging to the lute", in ROBERT DOWLAND: Varietie of lute-lessons [...], Thomas Adams, London 1610, paragraph "Of setting the right sizes of strings upon the lute".
7) Wellesley (Mass.), Wellesley College Library, "The Burwell lute tutor", manuscript ca. 1670, facsimile reprint with introduction by Robert Spencer, Boethius Press, Leeds 1973, the chapter 4 "Of the strings of the lute [...]".
8) THOMAS MACE: Musik's monument [...], the author & John Carr, London 1676, pp. 65-6.
9) At present it seems that only historical source that describe the bow's feel on the strings instead fingers is Galeazzi, p 72.
10) EPHRAIM SEGERMAN: âModern lute stringing and beliefs about gutâ, Fomrhi Quarterly, bull 98, January 2000, p.59.
11) SERAFINO DI COLCO: Lettera. prima (Venezia, 7 gennaro 1690), in Le vegghie di Minerva nella Accademia de Filareti: per il mese di gennaro 1690, Venezia 1690, pp. 32-3.
12) MARIN MERSENNE: Harmonie universelle [...], Livre quatriesme, Cramoisy, Paris 1636. Mersenne was the first that expained the relationship that exist between tension, gauge, string's scale and the string- density.
13) MARIN MERSENNE: Harmonie universelle [...], Livre quatriesme, Cramoisy, Paris 1636. Quoted by Stephen Bonta in 'Further thoughts on the history of strings'; Â The CatgutÂ Acoustical Society Newsletter nÂ° 26,Â November 1 , 1976, p 22..
14) ATTHANASIO KIRCHER: "Musurgia universalis [âŚ]", Lib V, 'De musica Instrumentali', p.440: " âŚdiversa soramina deducta in tantam deveniant subtilitatem, ut subtilissimi Capilli crassitiem adĂŚquentâ, Roma 1650.
15) See in PATRIZIO BARBIERI: âAcustica, Accordatura e Temperamento nellâilluminismo Veneto: con scritti inediti di Alessandro Barca, Giordano Riccati e altri Autoriâ, Istituto di Paleografia Musicale â Torre d'Orfeo, Roma 1987, p. 42.
16) Libro contenente la maniera di cucinare e vari segreti e rimedi per malattie et altro, manuscript, Reggio Emilia, Biblioteca Municipale Panizzi, Mss, vari E 177: "Corde da violino, modo di farle. Si prendino le budella di castrato o di capra fresche [...] volendo fare cantini se ne prende tre fila e si torgono al mulinelloâŚ"
17) Francois De Lalande, Voyage en Italie [âŚ] fait dans les annĂŠs 1765 & 1766, 2a edizione, vol IX, Desaint, Paris 1786, pp. 514-9, Chapire XXII âDu travail des Cordes Ă boyauxâŚ: â .
18) EPHRAIM SEGERMAN: âReview: Italian violin stringsâ, Fomrhi Quarterly, bull 98, January 2000, p.26-33 .
19) GIORDANO RICCATTI. Delle corde, ovvero fibre elastiche, Stamperia di San Tommaso d'Aquino, Bologna 1767, p. 130.
20) PATRIZIO BARBIERI : Roman and Neapolitan gut strings, 1550-1590, GSJ, May 2006, pp 176-7.
21) LEOPOLD MOZART: Versuch eine grĂźndlichen Violinscule [...], Verlag des Verfasser, Augsburg 1756, p.6.
22) For Savart see SEGERMAN: "Strings through the ages", part 2, p. 198.
23) FRANCOIS-JOSEPH FETIS: Antoine Stradivari luthier celĂ¨bre connu sous le nom de Stradivarivs [...], Vuillaume, Paris 1856, p. 92: acording to Jean-Baptiste Vuillaume' datas, from him we know that, 20 years before, the Violin's 1st was at 22 French pounds (11 kg ca.) of tension while the other strings were a bit less. The total tension was of 80 pounds (quoted by BARBIERI: "Giordano Riccati", p. 29)
24) CHARLES-EDOUARD-JOSEPH DELEZENNE: Experiences et observations sur les conies des instruments Ă archet, L. Danel, Lille 1853 (quited by BARBIERI: Acustica, accordatura e temperamento nellâ'illuminismo veneto, p.48). Folowing Barbieri, Delezenne at the beggining considered the equal tension idea but when he examined "ten different assortments of strings of commercial violin strings provided for him by the luthier Lapaix, finding instead average ratios [between the strings] noticeably lower than 1.5 [which was equal tension]": the Violin string gauges commonly available in the market measured by Delezenne: e'' = .61-.70; a' = .82-.96 mm; and d = 1.01-1.39 mm.
25)WILLIAM HUGGINS: "On the function of the sound-post and the proportional thickness of the strings on the violin", Royal Society proceeding, xxxv 1883, pp. 241-8: 248:
â The explanation of this departure of sizes of the strings which long experience has shown to be pratically most suitable, from the values they should have from theory, lies probably in the circumstance that the height of the bridge is different for the different strings. It is obvious, where the bridge is high, there is a greater downward pressure. There is also the circumstance that the string which go over a high part of the bridge stand farther from the finger-board, and have therefore to be pressed thorough a greater distance, would require more force than is required for the other strings, if the tension were not less.â.
26) JOSEPH-ANTOINE PLAISSARD: "Des cordes du violon", Association fracaise pour I'avancement des sciences. Congres del Lille, 187487 (quoted in BARBIERI: Acustica, accordatura e temperamento, p. 46.)
27) WILLIAM HUGGINS: "On the function of the sound-post", p. 248: "By means of a mechanical contrivance I found the weights necessary to deflect the strings to the same amount when the violin was in tune. The results agreed with the tensions which the sizes of the strings [i.e. corresponding to Ruffini's gauges] showed they would require to give fifths".
"Equal tension, Equal feel and Scaled tension" by Mimmo Peruffo is licensed under a Creative Commons Attribuzione-Non commerciale-Non opere derivate 3.0 Unported License.