S-expression/Advanced results: Difference between revisions
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== Using S-factorizations to understand the significance of S-expressions == | == Using S-factorizations to understand the significance of S-expressions == | ||
See [[S-expression#Using S-factorizations to understand the significance of S-expressions]]. | |||
== Mathematical derivations == | == Mathematical derivations == | ||
Latest revision as of 23:24, 26 May 2026
Using S-factorizations to understand the significance of S-expressions
See S-expression#Using S-factorizations to understand the significance of S-expressions.
Mathematical derivations
(Note for readers: Familiarity with basic algebra is advised, especially the rules (a + b)(a - b) = a2 - b2 and 1/(a/b) = b/a. Often multiple steps are combined into a single step for brevity, so follow carefully.)
For ultraparticulars, we want to show that Sk/S(k + 1) = ((k + 2)/(k - 1)) / ((k + 1)/k)3:
[math]\displaystyle{ \begin {align} {\rm S}k/{\rm S}(k + 1) &= \frac {k^2/(k^2 - 1)}{(k + 1)^2 / ((k + 1)^2 - 1)} \\ &= \frac {k^2}{(k + 1)(k - 1)} \cdot \frac{k^2 + 2k}{(k + 1)^2} \\ &= \frac {k^2}{(k + 1)^3 (k - 1)} \cdot (k + 2)k \\ &= \frac {k^3}{(k + 1)^3} \cdot \frac{(k + 2)}{(k - 1)} \\ &= \frac {(k + 2)/(k - 1)}{((k + 1)/k)^3} \end {align} }[/math]
For semiparticulars, we want to show that Sk/S(k + 2) = ((k + 3)/(k - 1)) / ((k + 2)/k)2:
[math]\displaystyle{ \begin {align} {\rm S}k/{\rm S}(k + 2) &= \frac {k^2/(k^2 - 1)}{(k + 2)^2 / ((k + 2)^2 - 1)} \\ &= \frac {k^2}{(k + 1)(k - 1)} \cdot \frac{(k + 3)(k + 1)}{(k + 2)^2} \\ &= \frac {k^2}{k - 1} \cdot \frac {k + 3}{(k + 2)^2} \\ &= \frac {k + 3}{k - 1} \cdot \frac{k^2}{(k + 2)^2} \\ &= \frac {(k + 3)/(k - 1)}{((k + 2)/k)^2} \end {align} }[/math]
For semiparticulars, we also want to show that Sk/S(k + 2) is superparticular for all but the case of S(4n - 1)/S(4n + 1) which is odd-particular:
[math]\displaystyle{ \begin {align} {\rm S}k/{\rm S}(k + 2) &= \frac {k + 3}{k - 1} \cdot \frac{k^2}{(k + 2)^2} \\ &= \frac {k^3 + 3k^2}{(k - 1)(k^2 + 4k + 4)} \\ &= \frac {k^3 + 3k^2}{k^3 + 4k^2 + 4k - k^2 - 4k - 4} \\ &= \frac {k^3 + 3k^2}{k^3 + 3k^2 - 4} \end {align} }[/math]
This result will be useful, so we will refer to it as [Eq. 1]: Sk/S(k + 2) = (k3 + 3k2)/(k3 + 3k2 - 4)
- Note that when k = 2n in [Eq. 1], everything in the numerator and denominator is divisible by 4 because the only instances of k have it raised to a power of 2 or greater meaning there will be a factor of (2n)2 = 4n2, therefore Sk/S(k + 2) is superparticular when k is even.
- When k = 4n + 1 in [Eq. 1], we have to do some extra work to show the result is superparticular:
- (4n + 1)3 = (4n)3 + 3·(4n)2 + 3·4n + 1 is of the form 4m + 1.
- (4n + 1)2 = (4n)2 + 2·4n + 1 is also of the form 4m + 1.
- Therefore we can replace their occurrences in [Eq. 1] with 4m + 1 and 4a + 1 respectively, without having to worry about what m and a are (as we only need to know that m and a are positive integers). Therefore to show S(4n + 1)/S(4n + 3) is superparticular, we set k = 4n + 1 in [Eq. 1] and then do the replacements and simplify to a superparticular:
- [math]\displaystyle{ \begin {align} {\rm S}(4n + 1)/{\rm S}(4n + 3) &= \frac {(4n + 1)^3 + 3(4n + 1)^2}{(4n + 1)^3 + 3(4n + 1)^2 - 4} \\ &= \frac {(4m + 1) + 3(4a + 1)}{(4m + 1) + 3(4a + 1) - 4} \\ &= \frac {4m + 4(3a) + 4}{4m + 4(3a)} \\ &= \frac {m + 3a + 1}{m + 3a} \end {align} }[/math]
- Then for the final case we want to show that S(4n - 1)/S(4n + 1) is odd-particular by setting k = 4n - 1 in [Eq. 1]:
- S(4n - 1)/S(4n + 1) = ( (4n - 1)3 + 3(4n - 1)2 )/( (4n - 1)3 + 3(4n - 1)2 - 4 )
- As before we make replacements:
- (4n - 1)3 = (4n)3 - 3·(4n)2 + 3·4n - 1 is of the form 4m - 1 so will be replaced with such.
- (4n + 1)2 = (4n)2 - 2·4n + 1 is of the form 4a + 1 so will be replaced with such.
- Therefore:
- [math]\displaystyle{ \begin {align} {\rm S}(4n - 1)/{\rm S}(4n + 1) &= \frac {(4n - 1)^3 + 3(4n - 1)^2}{(4n - 1)^3 + 3(4n - 1)^2 - 4} \\ &= \frac {(4m - 1) + 3(4a + 1)}{(4m - 1) + 3(4a + 1) - 4} \\ &= \frac {4m + 4(3a) + 2}{4m + 4(3a) - 2} \\ &= \frac {2m + 2(3a) + 1}{2m + 2(3a) - 1} \end {align} }[/math]
- … which is of the form (2x + 1)/(2x - 1) meaning it is odd-particular.
In conclusion: Sk/S(k + 2) is superparticular for k ≠ 3 (mod 4) and is odd-particular when k = 3 (mod 4).
Alternatively stated: S(k - 1)/S(k + 1) is superparticular for k ≠ 0 (mod 4) and is odd-particular when k = 0 (mod 4). This alternative statement highlights an interesting fact that the four harmonics related by tempering S(k - 1)/S(k + 1) are (k - 2):(k - 1):(k + 1):(k + 2) through tempering ((k+2)/(k-2)) / ((k+1)/(k-1))2 meaning the kth harmonic is the only one not included and therefore a semiparticular is odd-particular if the excluded "harmonic in the middle" (around which the two on each side are symmetric in terms of placement) is a multiple of 4 and is superparticular otherwise.
Abstraction
The maths
Let H be a commutative group with generators hi, ..., hk, ..., hj (such that i ≤ k ≤ j).
These generators are a series indexed by the integers that are analogous to a portion of the harmonic series, but "analogous" is extremely abstract here, because:
The fact that they are indexed by a range of integers is the only analogy that is guaranteed to hold, but as it turns out, is sufficient for defining analogies of superparticulars and thus S-expressions.
Thus: (the analogue of) a superparticular is of the form hk+1 hk-1 = hk+1 / hk (we'll use multiplicative notation) meaning that (the analogue of) Sk is:
[math]\displaystyle{ \begin {align} {\rm S}(k) = \frac{h_k^2}{h_{k-1} h_{k+1}} = (h_k / h_{k-1})/(h_{k+1} / h_k) = h_k h_{k-1}^{-1} (h_{k+1} h_k^{-1})^{-1} = h_k^2 h_{k-1}^{-1} h_{k+1}^{-1} \end {align} }[/math]
Then (the analogues of) S-factorizations correspond to the exponents of the generators, such that:
[math]\displaystyle{ \begin {align} {\rm S}(k) =\ .. h_{k-3}^0 h_{k-2}^0 h_{k-1}^{-1} h_k^2 h_{k+1}^{-1} h_{k+2}^0 h_{k+3}^0 ..\ = [..,\ h_{k-3},\ h_{k-2},\ h_{k-1},\ h_k,\ h_{k+1},\ h_{k+2},\ h_{k+3},\ ..]^{\Large[..,\ 0,\ 0, -1,\ 2, -1,\ 0,\ 0,\ ..]} \end {align} }[/math]
This completes the analogy. What this means is:
Every infinite comma family defined in terms of an S-expression will have an infinite number of analogues, because of the maths of S-factorizations continuing to work as expected.
The meanings of these analogues are up to us to interpret, however. This brings us to applications, which we will examine next, with a focus on the musical ones:
Applications
Unless otherwise specified, we will let k be in the positive integers (Z+) and we will let the group operation be the multiplication of rationals, but this abstraction is much more powerful than that.
If you are working with a certain expression for hk, it is suggested to use Sa where "a" is a letter that abbreviates the meaning of what you are using.
Letter suggestions are provided below for expressions suspected to be theoretically useful/interesting in the direction of designing desirable temperaments.
If we use the letter "a" for some analogy Sak, then because of the guarantees of the analogy, we will always be able to speak of a-square-particulars, a-ultraparticulars, a-semiparticulars, a-1/n-square-particulars and a-lopsided-commas, and have it make abstract sense.
To emphasize: this is because all comma families expressed in terms of expressions involving H's group operation applied to elements Sakp for k, p in Z will have analogues if k is a valid index for Sa.
Finally, while we usually speak of temperaments, note that S-expressions, as a tool for aiding RTT, have a wide variety of fruitful applications, exactly because RTT already itself has a wide variety of fruitful applications not explicitly involving tempering, especially in the design of scales where the constant structure property is desirable, where exotemperaments can shine as representing a deep, coarse logic.
hk = k
The trivial example, equal to normal S-expressions and S-factorizations, before abstraction.
hk = 2k + 1
An analogy of S-expressions and S-factorizations for EDTs which can be used as a corresponding RTT tool for when we only want to focus on the arithmetic of odds, using 3/1 as the new equave.
A suggestion is to use the notation Sok, if this is not unambiguous, with the letter "o" standing for "odd". Thus:
[math]\displaystyle{ \begin {align} {\rm So}(k) = h_k^2 h_{k-1}^{-1} h_{k+1}^{-1} = \frac{ (2k+1)^2 }{ (2k-1)(2k+3) } = \frac{ 4k^2 + 4k + 1 }{ 4k^2 + 4k - 3 } \end {align} }[/math]
hk = (k + 1)/k
An analogy of S-expressions and S-factorizations aiming at deeply faithful modelling of the harmonic series through modelling distances between superparticulars accurately.
A suggestion is to use the notation Ssk, if this is not unambiguous, with the letter "s" standing for "superparticular" or "super" generally.
We will see that this implies Ssk is the difference between two adjacent Sk (an ultraparticular), implying Ssk * Ss(k - 1) is a semiparticular. Thus:
[math]\displaystyle{ \begin {align} {\rm Ss}(k) = h_k^2 h_{k-1}^{-1} h_{k+1}^{-1} = \large \frac{ \frac{(k+1)}{k} \cdot \frac{(k+1)}{k} }{ \frac{k}{k-1}\cdot\frac{k+2}{k+1} } \normalsize = \frac{ {\rm S}(k+1) }{ {\rm S}(k) } \implies {\rm Ss}(k){\rm Ss}(k-1) = \frac{ {\rm S}(k+1) }{ {\rm S}(k) } \cdot \frac{ {\rm S}(k) }{ {\rm S}(k-1) } = \frac{ {\rm S}(k+1) }{ {\rm S}(k-1) } \end {align} }[/math]
This implies that s-ultraparticulars, s-semiparticulars, etc. are now about ratios between ultraparticulars, and that s-1/n-square-superparticulars are about ratios between square-particulars.
While the utility of the latter should be clear to those familiar with using square-particulars for analysis, it is not clear how useful a concept a ratio between ultraparticulars is, thus we should investigate why we might want such:
When we equate square-particulars, we lose accuracy the larger streak of them we equate, so eventually we are forced to break the chain.
When this happens, we have an ultraparticular that should, in any accurate temperament, be mapped positively, but as a result, we will have multiple such ultraparticulars.
Therefore, it is of interest to describe when these ultraparticulars are equated.
Now consider that as temperaments get more accurate, the streaks of equated square-particulars will either get higher/smaller or shorter, thus in the limit, we do not want to equate them.
Rather, we want to equate the ultraparticulars between them in order that we have a smooth growing of distances.
While the question of where it is most appropriate and accurate to equate ultraparticulars is beyond the scope of this section, it nonetheless shows that the 2D comma family Ssa/Ssb has utility.