Metallic MOS: Difference between revisions
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Scales based on this mean — or “phi”, as it is often called, after the Greek letter used to represent it — are relatively well-known, and these “golden” scales have been described by [[wikipedia:Erv_Wilson|Erv Wilson]], [[Kraig Grady|Kraig_Grady]], [http://www.elvenminstrel.com/music/tuning/horagrams/horagram_intro.htm David J. Finnamore], [https://ia800908.us.archive.org/31/items/mosedo.html/mosedo.html Billy Stiltner], [[wikipedia:Paul_Erlich|Paul Erlich]], [[Graham Breed|Graham Breed]], [[Dave Keenan|Dave Keenan]], [[Margo Schulter|Margo Schulter]], [[Das Goldene Tonsystem|Thorvald Kornerup]] and many others. | Scales based on this mean — or “phi”, as it is often called, after the Greek letter used to represent it — are relatively well-known, and these “golden” scales have been described by [[wikipedia:Erv_Wilson|Erv Wilson]], [[Kraig Grady|Kraig_Grady]], [http://www.elvenminstrel.com/music/tuning/horagrams/horagram_intro.htm David J. Finnamore], [https://ia800908.us.archive.org/31/items/mosedo.html/mosedo.html Billy Stiltner], [[wikipedia:Paul_Erlich|Paul Erlich]], [[Graham Breed|Graham Breed]], [[Dave Keenan|Dave Keenan]], [[Margo Schulter|Margo Schulter]], [[Das Goldene Tonsystem|Thorvald Kornerup]] and many others. | ||
But | But <span><math>φ</math></span> is only the first of an infinite continuum of such metallic means which can be used to generate scales offering interesting musical possibilities. And while some attention has been given to silver scales, what we seek to do here is centralize all met-MOS knowledge and generalize principles across all of the metallic means. | ||
The met-MOS concepts discussed here are abstract — unrelated to the octave, or neutral thirds, or any other size to which we might assign the period or generator. Being abstract, they only depend on the ratio between the period and the generator. Therefore we can set one of these two values to 1, for convenience, so that we only have to worry about the value of the other. We’ll be conforming here with the convention of setting the period to 1. | The met-MOS concepts discussed here are abstract — unrelated to the octave, or neutral thirds, or any other size to which we might assign the period or generator. Being abstract, they only depend on the ratio between the period and the generator. Therefore we can set one of these two values to 1, for convenience, so that we only have to worry about the value of the other. We’ll be conforming here with the convention of setting the period to 1. | ||
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=== Golden case === | === Golden case === | ||
The golden generator’s L:s sequence is simple. Every L:s ratio is | The golden generator’s L:s sequence is simple. Every L:s ratio is <span><math>φ</math></span>: | ||
<math>\qquad L:s = φ | <math>\qquad L:s = φ | ||
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=== Noble cases === | === Noble cases === | ||
A noble generator’s L:s sequence is slightly more complex. Not every — but almost every — L:s is | A noble generator’s L:s sequence is slightly more complex. Not every — but almost every — L:s is <span><math>φ</math></span>. Only the first few are not. | ||
=== Beyond golden cases === | === Beyond golden cases === | ||
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</math> | </math> | ||
But that’s not all. Due to the mathemagic of | But that’s not all. Due to the mathemagic of <span><math>φ</math></span>, we also get a recursive interval relationship pattern: | ||
<math> | <math> | ||
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Noble scales at first do not — but eventually do — reach a point where they start exhibiting this interval pattern (paralleling how their L:s sequences only eventually exhibit L:s = φ). | Noble scales at first do not — but eventually do — reach a point where they start exhibiting this interval pattern (paralleling how their L:s sequences only eventually exhibit L:s = φ). | ||
Once we’ve iterated past the point that our scale exhibits L:s = φ, some of the smaller intervals will begin to be related by | Once we’ve iterated past the point that our scale exhibits L:s = φ, some of the smaller intervals will begin to be related by <span><math>φ</math></span>, but its larger intervals will never be related by <span><math>φ</math></span>. | ||
=== Beyond golden cases === | === Beyond golden cases === | ||
The silver generator, as it did for its L:s sequence, alternates in quality between its two > 1 isotopes for its intervals. For half of its scales, | The silver generator, as it did for its L:s sequence, alternates in quality between its two > 1 isotopes for its intervals. For half of its scales, | ||
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</math> | </math> | ||
And as we can see, the ratio between those two lengths is | And as we can see, the ratio between those two lengths is <span><math>φ</math></span>: | ||
<math>\qquad \frac{0.618034}{0.381966} ≈ φ | <math>\qquad \frac{0.618034}{0.381966} ≈ φ | ||
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# begins the periodic phase of the L:s sequence for the metal they’re based on, and | # begins the periodic phase of the L:s sequence for the metal they’re based on, and | ||
# begins supporting the interval pattern for the metal they’re based on. | # begins supporting the interval pattern for the metal they’re based on. | ||
The golden generator is essentially the noble generator for the interval | The golden generator is essentially the noble generator for the interval <span><math>\frac 01</math></span> to <span><math>\frac 11</math></span>, which — being the root of the Stern-Brocot tree — is as golden as we can get: we see <span><math>L:s = φ</math></span> and <span><math>φ</math></span>'s distinctive interval pattern from the very start. | ||
And the noble generator between 0/1 and 1/3 | And the noble generator between 0/1 and 1/3 | ||
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</math> | </math> | ||
is very close to the root of the tree; it has initial L:s ratio of φ + 2, then attains L:s = φ after only one iteration. And it begins the golden interval pattern after just one iteration too. | is very close to the root of the tree; it has initial <span><math>L:s</math></span> ratio of <span><math>φ + 2</math></span>, then attains <span><math>L:s = φ</math></span> after only one iteration. And it begins the golden interval pattern after just one iteration too. | ||
On the other hand, the noble generator equal to 0.275267 — while only a smidgen off from the other noble generator we just looked at — necessitates iterating ''six'' times before attaining L:s = φ. This corresponds to it being the noble generator between 5/ | On the other hand, the noble generator equal to <span><math>0.275267</math></span> — while only a smidgen off from the other noble generator we just looked at — necessitates iterating ''six'' times before attaining <span><math>L:s = φ</math></span>. This corresponds to it being the noble generator between <span><math>\frac {5}{18}</math></span> and <span><math>\frac {3}{11}</math></span>, an interval which lies five levels deeper in the Stern-Brocot tree than the interval from <span><math>\frac 01</math></span> to <span><math>\frac 13</math></span>. | ||
So if we want a golden scale, and we also happen to want a generator near 0.276393, then we’re in luck. But if we want a golden generator that is close to 0.275267, we may be disappointed to hear that it is not “golden” enough for us. | So if we want a golden scale, and we also happen to want a generator near <span><math>0.276393</span></math>, then we’re in luck. But if we want a golden generator that is close to <span><math>0.275267</span></math>, we may be disappointed to hear that it is not “golden” enough for us. | ||
Wilson [http://www.anaphoria.com/hrgm.PDF documented noble scale sequences through the sixth level of the Stern-Brocot tree] (or as he called it, the “scale tree” or “Peirce Series”), totalling 32 noble generators. He also [http://anaphoria.com/sctree.pdf?fbclid=IwAR2PahVuZJ18faXQA_IggdD52y9PWP4uyEeQALE8Q73MhIlploPYDinbAAk recorded just the generator values down to the eleventh level] for a total of 1024 generators. Exploring generators beyond that was probably just not worth it, because their metallicity levels are too low. We will cut ourselves off at the seventh level in our scale trees, as we depict generators for the silver and bronze means, and their isotopes too. | Wilson [http://www.anaphoria.com/hrgm.PDF documented noble scale sequences through the sixth level of the Stern-Brocot tree] (or as he called it, the “scale tree” or “Peirce Series”), totalling 32 noble generators. He also [http://anaphoria.com/sctree.pdf?fbclid=IwAR2PahVuZJ18faXQA_IggdD52y9PWP4uyEeQALE8Q73MhIlploPYDinbAAk recorded just the generator values down to the eleventh level] for a total of 1024 generators. Exploring generators beyond that was probably just not worth it, because their metallicity levels are too low. We will cut ourselves off at the seventh level in our scale trees, as we depict generators for the silver and bronze means, and their isotopes too. | ||
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</math> | </math> | ||
This alone would not suffice to explain how the L:s sequences lock into a cycle of isotopes. But here’s where the magic of the metallic means comes into play. | This alone would not suffice to explain how the L:s sequences lock into a cycle of isotopes. But here’s where the magic of the metallic means comes into play. <span><math>φ</math></span> has the property that | ||
<math>\qquad φ - 1 = 1 / φ | <math>\qquad φ - 1 = 1 / φ | ||
</math> | </math> | ||
So, in the case of | So, in the case of <span><math>φ</math></span>: | ||
<math>\qquad L’:s’ = 1 / (L - 1) = 1 / (φ - 1) = 1 / (1 / φ) = φ | <math>\qquad L’:s’ = 1 / (L - 1) = 1 / (φ - 1) = 1 / (1 / φ) = φ | ||
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And that is why the isotopes less than 1 do not work for finding generators: they are redundant with their respective metallic mean. | And that is why the isotopes less than 1 do not work for finding generators: they are redundant with their respective metallic mean. | ||
For example, the golden mean does have an isotope, ≈ 0.618034, however, because | For example, the golden mean does have an isotope, ≈ 0.618034, however, because the golden mean minus one is the same as the inverse of the golden mean, | ||
<math>\qquad 1:φ = (φ - 1):1 | <math>\qquad 1:φ = (φ - 1):1 | ||
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</math> | </math> | ||
We’ve stated that L:s = φ for every golden scale, while L:s for noble scales eventually do, just not at first. Noble L:s sequences lock onto | We’ve stated that <span><math>L:s = φ</math></span> for every golden scale, while L:s for noble scales eventually do, just not at first. Noble L:s sequences lock onto <span><math>φ</math></span> at the point where depleting the continued fraction more no longer changes it (removing a <span><math>1</math></span> from the beginning of an infinite string of <span><math>1</math></span>’s is a no-op). | ||
Thus it makes sense that logarithmic phi’s L:s sequence remains fixed from the beginning, because with a continued fraction of [0; 1] we get the L:s sequence | Thus it makes sense that logarithmic phi’s L:s sequence remains fixed from the beginning, because with a continued fraction of <span><math>[0; 1]</span></math> we get the L:s sequence | ||
<math> | <math> | ||
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(L+s):L = φ | (L+s):L = φ | ||
In other words, any interval in the scale which spans exactly one large and one small step is | In other words, any interval in the scale which spans exactly one large and one small step is <span><math>φ</math></span> times the size of one large step. | ||
This fact follows from one of the many ways of defining the golden mean: the value for which | This fact follows from one of the many ways of defining the golden mean: the value for which | ||
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Find any s in the horogram and observe how it gets split up as we iterate through the scale sequence. In the next iteration, s will be replaced with L. After two iterations, the original s interval is now represented by an L and an s. And so forth. | Find any s in the horogram and observe how it gets split up as we iterate through the scale sequence. In the next iteration, s will be replaced with L. After two iterations, the original s interval is now represented by an L and an s. And so forth. | ||
Every MOS scale contains every scale earlier in its scale sequence. In other words, any interval that existed in an earlier scale will remain in all later scales. These earlier L’s and s’s that remain — only now spanning many L’s and s’s each — are precisely the larger intervals in the scale that also exhibit the | Every MOS scale contains every scale earlier in its scale sequence. In other words, any interval that existed in an earlier scale will remain in all later scales. These earlier L’s and s’s that remain — only now spanning many L’s and s’s each — are precisely the larger intervals in the scale that also exhibit the <span><math>φ</math></span> ratio to each other. | ||
=== Beyond golden cases === | === Beyond golden cases === | ||
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== Golden Meantone == | == Golden Meantone == | ||
The thinking behind [[Golden Meantone]] is to put the whole step and half step into the ratio of | The thinking behind [[Golden Meantone]] is to put the whole step and half step into the ratio of <span><math>φ</math></span> with each other. Most discussion of Golden Meantone assumes a twelve-note scale that spans an octave. | ||
Abstractly speaking, Golden Meantone’s generator is a noble generator weighted by | Abstractly speaking, Golden Meantone’s generator is a noble generator weighted by <span><math>φ</math></span> from <span><math>\frac 13</math></span> toward <span><math>\frac 12</math></span>, ≈ 0.419821, which by design was the one chosen for all noble generator examples in this discussion. | ||
Wilson called this scale [http://anaphoria.com/kornerup.pdf?fbclid=IwAR3nAiMo-W51E5IT5vXxmMFBIsSocPu6tAr4ETbQF-ITrxvoakAR11DpM_4 Kornerup], after Thorvald Kornerup, who was an early explorer of golden scales. | Wilson called this scale [http://anaphoria.com/kornerup.pdf?fbclid=IwAR3nAiMo-W51E5IT5vXxmMFBIsSocPu6tAr4ETbQF-ITrxvoakAR11DpM_4 Kornerup], after Thorvald Kornerup, who was an early explorer of golden scales. | ||
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== Wilson/Pepper Fifth Tuning == | == Wilson/Pepper Fifth Tuning == | ||
The thinking behind this tuning is similar, except that the two steps in the ratio of | The thinking behind this tuning is similar, except that the two steps in the ratio of <span><math>φ</math></span> with each other are the tone and the chromatic semitone. | ||
Abstractly speaking, Wilson/Pepper Fifth Tuning’s generator would be the noble generator weighted by | Abstractly speaking, Wilson/Pepper Fifth Tuning’s generator would be the noble generator weighted by <span><math>φ</math></span> from <span><math>\frac 37</math></span> to <span><math>\frac 25</math></span>, <span><math>≈ 0.413254</math></span>. | ||
== Argent Temperament == | == Argent Temperament == | ||
[[File:Argent horogram.png|alt=horogram for g = 0.414214, 7 iterations|right|388x388px]] | [[File:Argent horogram.png|alt=horogram for g = 0.414214, 7 iterations|right|388x388px]] | ||
Scales based on the bronze mean and metallic means beyond it have not been extensively explored. However, the silver mean has gotten some attention. | Scales based on the bronze mean and metallic means beyond it have not been extensively explored. However, the silver mean has gotten some attention. | ||
Most discussion of Argent Temperament — like Golden Meantone — assumes an octave period; the thinking behind it is to put the fifth and the fourth into the ratio of | Most discussion of Argent Temperament — like Golden Meantone — assumes an octave period; the thinking behind it is to put the fifth and the fourth into the ratio of <span><math>\sqrt{2}</math></span> with each other. The justly tuned versions of these intervals, <span><math>\frac 32</math></span> and <span><math>\frac 43</math></span>, respectively, are remarkably close to this already, only off by a fiftieth of a cent: | ||
{| class="wikitable" | {| class="wikitable" | ||
|interval | |interval | ||
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So in our terms, this would be an isotopic generator, and again, by design, this was the isotopic generator chosen for examples in this discussion, ≈ 0.414214. | So in our terms, this would be an isotopic generator, and again, by design, this was the isotopic generator chosen for examples in this discussion, ≈ 0.414214. | ||
It may seem odd that the most popular use of the silver mean uses its isotope rather than the mean directly. However, if we consider the ratio of the generator to the period here, that ratio is the silver mean. In the golden case, there was no difference between these two conceptions; both splitting the period into two segments in the ratio of | It may seem odd that the most popular use of the silver mean uses its isotope rather than the mean directly. However, if we consider the ratio of the generator to the period here, that ratio is the silver mean. In the golden case, there was no difference between these two conceptions; both splitting the period into two segments in the ratio of <span><math>φ</math></span> and having the generator to period ratio be <span><math>φ</math></span> produce the same result. So while in this discussion from the beginning we put things in terms of splitting intervals (in order to smoothly transition from the golden generator into noble generators), it is probably the case that those who first brought us the Fibonacci generator and Argent Temperament were thinking in terms of the ratio of the generator to the period. | ||
Argent means “silver” in French, which explains the name (it has also been called Arguros, which is “silver” in Greek). Wilson called this generator 2-Zig/2-Zag, after the pattern of the lines in the Stern-Brocot tree that results as we traverse deeper into the tree searching for better approximations of it: we move twice to the right, then twice to the left, and repeat. | Argent means “silver” in French, which explains the name (it has also been called Arguros, which is “silver” in Greek). Wilson called this generator 2-Zig/2-Zag, after the pattern of the lines in the Stern-Brocot tree that results as we traverse deeper into the tree searching for better approximations of it: we move twice to the right, then twice to the left, and repeat. | ||
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The two segments are actually in a ratio equal to the weight multiplied by the ratio of the denominators of their respective bounds. | The two segments are actually in a ratio equal to the weight multiplied by the ratio of the denominators of their respective bounds. | ||
We’ll test this out on the example from before. We know that the weighted mediant formula with | We’ll test this out on the example from before. We know that the weighted mediant formula with <span><math>φ</math></span> as weight, the interval between 1/3 and 1/2, and weight leaning toward the parent ratio (1/2) gives the value 0.419821. So our two segments are: | ||
<math> | <math> | ||
| Line 1,050: | Line 1,053: | ||
The fact that the numerators do not figure into the result at all speaks to the impossibility of finding more than one interval on the tree with the same two bounding ratio denominators. | The fact that the numerators do not figure into the result at all speaks to the impossibility of finding more than one interval on the tree with the same two bounding ratio denominators. | ||
We can also infer why the ratio worked out to exactly | We can also infer why the ratio worked out to exactly <span><math>φ</math></span> in the case of the entire period: both of the denominators of 0/1 and 1/1 are 1, so the scalar on <span><math>φ</math></span> was 1. | ||
And from this we also ascertain that weighted mediants sometimes fall toward the edges of the interval and sometimes toward the middle. I.e. if we choose the interval 8/21 to 5/13, weighted by | And from this we also ascertain that weighted mediants sometimes fall toward the edges of the interval and sometimes toward the middle. I.e. if we choose the interval 8/21 to 5/13, weighted by <span><math>φ</math></span> toward 5/13, the ratio between the two split segments would be 13φ/21 = 1.001640, making that split almost right down the middle; on the other hand, if we chose the interval 0/1 to 1/7, weighted by <span><math>φ</math></span> toward 1/7, the ratio between the two split segments would be 7φ/1 = 11.326238, extremely off. | ||
== Generator introduction counts == | == Generator introduction counts == | ||